Publications
Show :: Close all abstracts
2023 : 2022 : 2021 : 2020 : 2019 : 2018 :2017 : 2016 : 2015 : 2014 : 2013 : 2012 : 2011 : 2010 : 2009 & earlier
- A. Ungar, P. Cappellaro, A. Cooper and W. K. C. Sun "Control of an Environmental Spin Defect beyond the Coherence Limit of a Central Spin"
- G. Wang, W. Xu, C. Li, V. Vuletić and P. Cappellaro "Individual-atom control in array through phase modulation"
- G. Wang, M.-T. Nguyen, D. W. deQuilettes , E. Price, Z. Hu, D. A. Braje and P. Cappellaro "Emulated nuclear spin gyroscope with 15NV centers in diamond"
- G. Wang, M.-T. Nguyen and P. Cappellaro "Hyperfine-enhanced gyroscope based on solid-state spins"
- H. Tang, G. Wang, P. Cappellaro and J. Li "μeV-deep neutron bound states in nanocrystals"
- H. Xu, U. Delić, G. Wang, C. Li, P. Cappellaro and J. Li "Exponentially Enhanced non-Hermitian Cooling"
- A. Stasiuk, P. Peng, G. Heller and P. Cappellaro "Frame Change Technique for Phase Transient Cancellation"
- R. Budakian, A. Finkler, A. Eichler, M. Poggio, C. L. Degen, S. Tabatabaei, I. Lee, P. C. Hammel, E. S. Polzik, T. H. Taminiau, R. L. Walsworth, P. London, A. B. Jayich, A. Ajoy, A. Pillai, J. Wrachtrup, F. Jelezko, Y. Bae, A. J. Heinrich, C. R. Ast, P. Bertet, P. Cappellaro, C. Bonato, Y. Altmann and E. Gauger "Roadmap on Nanoscale Magnetic Resonance Imaging"
- C. Li, B. Li, O. Amer, R. Shaydulin, S. Chakrabarti, G. Wang, H. Xu, H. Tang, I. Schoch, N. Kumar, C. Lim, J. Li, P. Cappellaro and M. Pistoia "Blind quantum machine learning with quantum bipartite correlator"
- H. Xu, C. Li, G. Wang, H. Tang, P. Cappellaro and J. Li "Efficient Quantum Transduction Using Anti-Ferromagnetic Topological Insulators"
- C. Li, S.-X. L. Luo, D. M. Kim, G. Wang and P. Cappellaro "Ion sensors with crown ether-functionalized nanodiamonds"
- S. Hernández-Gómez, F. Balducci, G. Fasiolo, P. Cappellaro, N. Fabbri and A. Scardicchio "Optimal control of a quantum sensor: A fast algorithm based on an analytic solution"
- C. Li, M. Chen and P. Cappellaro "A geometric perspective: experimental evaluation of the quantum Cramer-Rao bound"
- A. Stasiuk and P. Cappellaro "Observation of a Prethermal U(1) Discrete Time Crystal"
- A. Ameri, E. Ye, P. Cappellaro, H. Krovi and N. F. Loureiro "Quantum algorithm for the linear Vlasov equation with collisions"
- G. Wang, A. R. Barr, H. Tang, M. Chen, C. Li, H. Xu, A. Stasiuk, J. Li and P. Cappellaro "Characterizing Temperature and Strain Variations with Qubit Ensembles for Their Robust Coherence Protection"
- H. Tang, A. R. Barr, G. Wang, P. Cappellaro and J. Li "First-Principles Calculation of the Temperature-Dependent Transition Energies in Spin Defects"
- G. Wang, C. Li, H. Tang, B. Li, F. Madonini, F. F. Alsallom, W. K. C. Sun, P. Peng, F. Villa, J. Li and P. Cappellaro "Manipulating solid-state spin concentration through charge transport"
- H. Tang, B. Li, G. Wang, H. Xu, C. Li, A. Barr, P. Cappellaro and J. Li "Communication-Efficient Quantum Algorithm for Distributed Machine Learning"
- H. Xu, H. Tang, G. Wang, C. Li, B. Li, P. Cappellaro and J. Li "Solid-state 229Th nuclear laser with two-photon pumping"
- G. Wang, F. Madonini, B. Li, C. Li, J. Xiang, F. Villa and P. Cappellaro "Fast Wide-Field Quantum Sensor Based on Solid-State Spins Integrated with a SPAD Array"
- P. Peng, B. Ye, Yao Norman Y. and P. Cappellaro "Exploiting disorder to probe spin and energy hydrodynamics"
- H. Xu, C. Li, G. Wang, H. Wang, H. Tang, A. R. Barr, P. Cappellaro and J. Li "Two-Photon Interface of Nuclear Spins Based on the Optonuclear Quadrupolar Effect"
- H. Xu, G. Wang, C. Li, H. Wang, H. Tang, A. R. Barr, P. Cappellaro and J. Li "Laser Cooling of Nuclear Magnons"
- M. Chen, C. Li, G. Palumbo, Y.-Q. Zhu, N. Goldman and P. Cappellaro "A synthetic monopole source of Kalb-Ramond field in diamond"
- G. Wang, Y.-X. Liu, J. M. Schloss, S. T. Alsid, D. A. Braje and P. Cappellaro "Sensing of Arbitrary-Frequency Fields Using a Quantum Mixer"
- I. Rojkov, D. Layden, P. Cappellaro, J. Home and F. Reiter "Bias in Error-Corrected Quantum Sensing"
- S. Hernández-Gómez, S. Gherardini, N. Staudenmaier, F. Poggiali, M. Campisi, A. Trombettoni, F. Cataliotti, P. Cappellaro and N. Fabbri "Autonomous Dissipative Maxwell's Demon in a Diamond Spin Qutrit"
- P. Peng, X. Huang, C. Yin, L. Joseph, C. Ramanathan and P. Cappellaro "Deep Reinforcement Learning for Quantum Hamiltonian Engineering"
- W. K. C. Sun and P. Cappellaro "Self-consistent noise characterization of quantum devices"
- Changhao Li, Rouhollah Soleyman, Mohammad Kohandel, and Paola Cappellaro "SARS-CoV-2 Quantum Sensor Based on Nitrogen-Vacancy Centers in Diamond"
- G. Wang, Y.-X. Liu, Y. Zhu and P. Cappellaro "Nanoscale Vector AC Magnetometry with a Single Nitrogen-Vacancy Center in Diamond"
- G. Wang, C. Li and P. Cappellaro "Observation of symmetry-protected selection rules in periodically driven quantum systems"
- P. Peng, C. Yin, X. Huang, C. Ramanathan and P. Cappellaro "Floquet prethermalization in dipolar spin chains"
- C. Li, T. Li, Y.-X. Liu and P. Cappellaro "Effective routing design for remote entanglement generation on quantum networks"
- G. Wang, Y.-X. Liu and P. Cappellaro "Observation of the high-order Mollow triplet by quantum mode control with concatenated continuous driving"
- C. Yin, P. Peng, X. Huang, C. Ramanathan and P. Cappellaro "Prethermal quasiconserved observables in Floquet quantum systems"
- G. Wang, Y.-X. Liu and P. Cappellaro "Coherence protection and decay mechanism in qubit ensembles under concatenated continuous driving"
- A. Sone, Y.-X. Liu and P. Cappellaro "Quantum Jarzynski Equality in Open Quantum Systems from the One-Time Measurement Scheme"
- S. Hernández-Gómez, S. Gherardini, F. Poggiali, F. S. Cataliotti, A. Trombettoni, P. Cappellaro and N. Fabbri "Experimental test of exchange fluctuation relations in an open quantum system"
- Y.-X. Liu, J. Hines, Z. Li, A. Ajoy and P. Cappellaro "High-fidelity Trotter formulas for digital quantum simulation"
- H. Zhou, J. Choi, S. Choi, R. Landig, A. M. Douglas, J. Isoya, F. Jelezko, S. Onoda, H. Sumiya, P. Cappellaro, H. S. Knowles, H. Park and M. D. Lukin "Quantum Metrology with Strongly Interacting Spin Systems"
- S. Hernandez-Gomez, F. Poggiali, N. Fabbri, P. Cappellaro "Environment spectroscopy with an NV center in diamond"
- A. Cooper, W. K. C. Sun, J.-C. Jaskula and P. Cappellaro "Identification and Control of Electron-Nuclear Spin Defects in Diamond"
- D. Layden, M. Chen and P. Cappellaro "Efficient Quantum Error Correction of Dephasing Induced by a Common Fluctuator"
- C. M. Sánchez, A. K. Chattah, K. X. Wei, L. Buljubasich, P. Cappellaro and H. M. Pastawski "Perturbation Independent Decay of the Loschmidt Echo in a Many-Body System"
- W. K. C. Sun, A. Cooper and P. Cappellaro "Improved entanglement detection with subspace witnesses"
- D. Layden, L. R. Huang and P. Cappellaro "Robustness-optimized quantum error correction"
- G. Liu, M. Chen, Y.-X. Liu, D. Layden and P. Cappellaro "Repetitive readout enhanced by machine learning"
- Y. Wang, D. Dong, A. Sone, I. R. Petersen, H. Yonezawa and P. Cappellaro "Quantum Hamiltonian Identifiability via a Similarity Transformation Approach and Beyond"
- P. Peng, Z. Li, H. Yan, K. X. Wei and P. Cappellaro "Comparing many-body localization lengths via non-perturbative construction of local integrals of motion"
- C. Li and P. Cappellaro "Telecom photon interface of solid-state quantum nodes"
- C. Li, M. Chen, D. Lyzwa and P. Cappellaro "All-Optical Quantum Sensing of Rotational Brownian Motion of Magnetic Molecules"
- A. Cooper, W. K. C. Sun, J.-C. Jaskula and P. Cappellaro "Environment-assisted Quantum-enhanced Sensing with Electronic Spins in Diamond"
- J.-C. Jaskula, K. Saha, A. Ajoy, D. J. Twitchen, M. Markham and P. Cappellaro "Cross-sensor feedback stabilization of an emulated quantum spin gyroscope"
- S. Zhou, D. Layden, M. Zhang, J. Preskill, P. Cappellaro and L. Jiang "Error-corrected quantum sensing"
- A. Sone, Q. Zhuang, C. Li, Y.-X. Liu and P. Cappellaro "Nonclassical correlations for quantum metrology in thermal equilibrium"
- F. Poggiali, S. Hernández-Gómez, P. Cappellaro and N. Fabbri "Optimal control of diamond spin qubits for quantum sensing in noisy environments"
- Y.-X. Liu, A. Ajoy and P. Cappellaro "Nanoscale Vector dc Magnetometry via Ancilla-Assisted Frequency Up-Conversion"
- A. Ajoy, U. Bissbort, D. Poletti and P. Cappellaro "Selective Decoupling and Hamiltonian Engineering in Dipolar Spin Networks"
- D. Layden, S. Zhou, P. Cappellaro and L. Jiang "Ancilla-Free Quantum Error Correction Codes for Quantum Metrology"
- K. X. Wei, P. Peng, O. Shtanko, I. Marvian, S. Lloyd, C. Ramanathan and P. Cappellaro "Emergent Prethermalization Signatures in Out-of-Time Ordered Correlations"
- M. Chen, W. K. C. Sun, K. Saha, J.-C. Jaskula and P. Cappellaro "Protecting solid-state spins from a strongly coupled environment"
- S. Hernández-Gómez, F. Poggiali, P. Cappellaro and N. Fabbri "Noise spectroscopy of a quantum-classical environment with a diamond qubit"
- M. Hirose and P. Cappellaro "Time-optimal control with finite bandwidth"
- D. Layden and P. Cappellaro "Spatial noise filtering through error correction for quantum sensing"
- L. Marseglia, K. Saha, A. Ajoy, T. Schroeder, D. Englund, F. Jelezko, R. Walsworth, J. L. Pacheco, D. L. Perry, E. S. Bielejec and P. Cappellaro "Bright nanowire single photon source based on SiV centers in diamond"
- F. Poggiali, P. Cappellaro and N. Fabbri "Optimal Control for One-Qubit Quantum Sensing"
- A. Sone, Q. Zhuang and P. Cappellaro "Quantifying precision loss in local quantum thermometry via diagonal discord"
- K. X. Wei, C. Ramanathan and P. Cappellaro "Exploring Localization in Nuclear Spin Chains"
- A. Ajoy, Y.-X. Liu, K. Saha, L. Marseglia, J.-C. Jaskula, U. Bissbort and P. Cappellaro "Quantum interpolation for high-resolution sensing"
- S. T. Alsid "Optimizing chemical-vapor-deposition diamond for nitrogen-vacancy center ensemble magnetometry"
- A. Sone and P. Cappellaro "Hamiltonian identifiability assisted by a single-probe measurement"
- A. Sone and P. Cappellaro "Exact dimension estimation of interacting qubit systems assisted by a single quantum probe"
- C. L. Degen, F. Reinhard and P. Cappellaro "Quantum sensing"
- F. Poggiali, P. Cappellaro and N. Fabbri "Measurement of the excited-state transverse hyperfine coupling in NV centers via dynamic nuclear polarization"
- L. Marseglia, K. Saha, A. Ajoy, T. Schroder, D. R. Englund, T. TERAJI, junichi isoya, F. Jelezko, R. Walsworth, J. L. Pacheco, D. Perry, E. Bielejec and P. Cappellaro "A bright nanowire single photon source"
- A. Ajoy "Quantum Assisted Sensing, Simulation and Control"
- A. Cooper-Roy "Coherent control of electron spins in diamond for quantum information science and quantum sensing"
- M. Hirose and P. Cappellaro "Coherent feedback control of a single qubit in diamond"
- L. M. Pham, S. J. DeVience, F. Casola, I. Lovchinsky, A. O. Sushkov, E. Bersin, J. Lee, E. Urbach, P. Cappellaro, H. Park, A. Yacoby, M. Lukin and R. L. Walsworth "NMR technique for determining the depth of shallow nitrogen-vacancy centers in diamond"
- M. Chen, M. Hirose and P. Cappellaro "Measurement of transverse hyperfine interaction by forbidden transitions"
- K. Arai, C. Belthangady, H. Zhang, N. Bar-Gill, S. DeVience, P. Cappellaro, A. Yacoby and R. Walsworth "Fourier magnetic imaging with nanoscale resolution and compressed sensing speed-up using electronic spins in diamond"
- C. Aiello, M. Allegra, B. Hemmerling, X. Wan and P. Cappellaro "Algebraic synthesis of time-optimal unitaries in SU(2) with alternating controls"
- P. Cappellaro "Polarizing Nuclear Spins in Silicon Carbide"
- A. Ajoy, U. Bissbort, M. D. Lukin, R. L. Walsworth and P. Cappellaro "Atomic-Scale Nuclear Spin Imaging Using Quantum-Assisted Sensors in Diamond"
- C. D. Aiello and P. Cappellaro "Time-optimal control by a quantum actuator"
- M. Hirose "Quantum Control of Spin Systems in diamond"
- N. Lopez "All-Optical Method of Nanoscale Magnetometry for Ensembles of Nitrogen-Vacancy Defects in Diamond"
- A. Cooper, E. Magesan, H. Yum and P. Cappellaro "Time-resolved magnetic sensing with electronic spins in diamond"
- P. Cappellaro "Implementation of State Transfer Hamiltonians in Spin Chains with Magnetic Resonance Techniques"
- C. D. Aiello "Qubit Dynamics under Alternating Controls"
- E. Magesan, A. Cooper and P. Cappellaro "Compressing measurements in quantum dynamic parameter estimation,"
- C. D. Aiello, M. Hirose and P. Cappellaro "Composite-pulse magnetometry with a solid-state quantum sensor"
- A. Ajoy and P. Cappellaro "Perfect quantum transport in arbitrary spin networks"
- A. Ajoy and P. Cappellaro "Quantum simulation via filtered Hamiltonian engineering: application to perfect quantum transport in spin networks"
- C. Belthangady, N. Bar-Gill, L. M. Pham, K. Arai, D. Le Sage, P. Cappellaro and R. L. Walsworth "Dressed-State Resonant Coupling between Bright and Dark Spins in Diamond"
- G. Kaur, A. Ajoy and P. Cappellaro "Decay of spin coherences in one-dimensional spin systems"
- E. Magesan, A. Cooper, H. Yum and P. Cappellaro "Reconstructing the profile of time-varying magnetic fields with quantum sensors"
- E. Magesan and P. Cappellaro "Experimentally efficient methods for estimating the performance of quantum measurements"
- A. Ajoy and P. Cappellaro "Mixed-state quantum transport in correlated spin networks"
- A. Ajoy and P. Cappellaro "Stable three-axis nuclear-spin gyroscope in diamond"
- N. Bar-Gill, L. Pham, C. Belthangady, D. Le Sage, P. Cappellaro, J. Maze, M. Lukin, A. Yacoby and R. Walsworth "Suppression of spin-bath dynamics for improved coherence of multi-spin-qubit systems"
- P. Cappellaro "Spin-bath narrowing with adaptive parameter estimation"
- P. Cappellaro, G. Goldstein, J. S. Hodges, L. Jiang, J. R. Maze, A. S. Sørensen and M. D. Lukin "Environment-assisted metrology with spin qubits"
- M. Hirose, C. D. Aiello and P. Cappellaro "Continuous dynamical decoupling magnetometry"
- G. Kaur and P. Cappellaro "Initialization and readout of spin chains for quantum information transport"
- L. M. Pham, N. Bar-Gill, C. Belthangady, D. Le Sage, P. Cappellaro, M. D. Lukin, A. Yacoby and R. L. Walsworth "Enhanced solid-state multispin metrology using dynamical decoupling"
- F. Ticozzi, R. Lucchese, P. Cappellaro and L. Viola "Hamiltonian Control of Quantum Dynamical Semigroups: Stabilization and Convergence Speed"
- P. Cappellaro, L. Viola and C. Ramanathan "Coherent-state transfer via highly mixed quantum spin chains"
- G. Goldstein, P. Cappellaro, J. R. Maze, J. S. Hodges, L. Jiang, A. S. Sørensen and M. D. Lukin "Environment Assisted Precision Measurement"
- L. M. Pham, D. Le Sage, P. L. Stanwix, T. K. Yeung, D. Glenn, A. Trifonov, P. Cappellaro, P. R. Hemmer, M. D. Lukin, H. Park, A. Yacoby and R. L. Walsworth "Magnetic field imaging with nitrogen-vacancy ensembles"
- C. Ramanathan, P. Cappellaro, L. Viola and D. G. Cory "Experimental characterization of coherent magnetization transport in a one-dimensional spin system"
- C. Altafini, P. Cappellaro and D. Cory "Feedback schemes for radiation damping suppression in NMR: A control-theoretical perspective"
- G. Goldstein, M. D. Lukin and P. Cappellaro "Quantum Limits on Parameter Estimation"
- C. A. Meriles, L. Jiang, G. Goldstein, J. S. Hodges, J. Maze, M. D. Lukin and P. Cappellaro "Imaging mesoscopic nuclear spin noise with a diamond magnetometer"
- P. L. Stanwix, L. M. Pham, J. R. Maze, D. Le Sage, T. K. Yeung, P. Cappellaro, P. R. Hemmer, A. Yacoby, M. D. Lukin and R. L. Walsworth "Coherence of nitrogen-vacancy electronic spin ensembles in diamond"
- C. Altafini, P. Cappellaro and D. Cory "Feedback schemes for radiation damping suppression in NMR: a control-theoretical perspective"
- P. Cappellaro, L. Jiang, J. S. Hodges and M. D. Lukin "Coherence and Control of Quantum Registers Based on Electronic Spin in a Nuclear Spin Bath"
- P. Cappellaro and M. D. Lukin "Quantum correlation in disordered spin systems: Applications to magnetic sensing"
- P. Cappellaro, J. Maze, L. Childress, M. Dutt, J. Hodges, S. Hong, L. Jiang, P. Stanwix, J. Taylor, E. Togan and others "Quantum Control of Spins and Photons at Nanoscales"
- J. R. Maze, P. Cappellaro, L. Childress, M. V. G. Dutt, J. S. Hodges, S. Hong, L. Jiang, P. L. Stanwix, J. M. Taylor, E. Togan, A. S. Zibrov, P. Hemmer, A. Yacoby, R. L. Walsworth and M. D. Lukin "Nanoscale magnetic sensing using spin qubits in diamond"
- P. Rabl, P. Cappellaro, M. V. G. Dutt, L. Jiang, J. R. Maze and M. D. Lukin "Strong magnetic coupling between an electronic spin qubit and a mechanical resonator"
- W. Zhang, P. Cappellaro, N. Antler, B. Pepper, D. G. Cory, V. V. Dobrovitski, C. Ramanathan and L. Viola "NMR multiple quantum coherences in quasi-one-dimensional spin systems: Comparison with ideal spin-chain dynamics"
- L. Jiang, M. V. G. Dutt, E. Togan, L. Childress, P. Cappellaro, J. M. Taylor and M. D. Lukin "Coherence of an Optically Illuminated Single Nuclear Spin Qubit"
- J. R. Maze, P. L. Stanwix, J. S. Hodges, S. Hong, J. M. Taylor, P. Cappellaro, L. Jiang, A. Zibrov, A. Yacoby, R. Walsworth and M. D. Lukin "Nanoscale magnetic sensing with an individual electronic spin qubit in diamond"
- J. M. Taylor, P. Cappellaro, L. Childress, L. Jiang, D. Budker, P. R. Hemmer, A. Yacoby, R. Walsworth and M. D. Lukin "High-sensitivity diamond magnetometer with nanoscale resolution"
- P. Cappellaro, J. S. Hodges, T. F. Havel and D. G. Cory "Subsystem pseudopure states"
- P. Cappellaro, C. Ramanathan and D. G. Cory "Dynamics and control of a quasi-one-dimensional spin system"
- P. Cappellaro, C. Ramanathan and D. G. Cory "Simulations of Information Transport in Spin Chains"
- P. Cappellaro, J. S. Hodges, T. F. Havel and D. G. Cory "Control of qubits encoded in decoherence-free subspaces"
- J. S. Hodges, P. Cappellaro, T. F. Havel, R. Martinez and D. G. Cory "Experimental implementation of a logical Bell state encoding"
- P. Cappellaro, J. S. Hodges, T. F. Havel and D. G. Cory "Principles of Control for Decoherence-Free Subsystems"
- P. Cappellaro, J. Emerson, N. Boulant, C. Ramanathan, S. Lloyd and D. G. Cory "Spin amplifier for single spin measurement"
- P. Cappellaro "Quantum Information Processing in Multi-Spin Systems"
- H. J. Cho, P. Cappellaro, D. G. Cory and C. Ramanathan "Decay of highly correlated spin states in a dipolar-coupled solid: NMR study of CaF2"
- J. Hodges, P. Cappellaro, T. Havel and D. Cory "Quantum Control of Nuclear Spins"
- C. A. Perez-Delgado, M. Mosca, P. Cappellaro and D. G. Cory "Single Spin Measurement Using Cellular Automata Techniques"
- P. Cappellaro, J. Emerson, N. Boulant, C. Ramanathan, S. Lloyd and D. G. Cory "Entanglement Assisted Metrology"
- T. Havel, P. Cappellaro, C. Ramanathan and D. Cory "Quantum Information Processing with Nuclear Spin-Based Devices"
- G. S. Boutis, P. Cappellaro, H. Cho, C. Ramanathan and D. G. Cory "Pulse error compensating symmetric magic-echo trains"
- C. Ramanathan, H. Cho, P. Cappellaro, G. S. Boutis and D. G. Cory "Encoding multiple quantum coherences in non-commuting bases"
- C. Ramanathan, H. Cho, P.Cappellaro, G.S. Boutis and D. Cory "Exploring large nuclear spin systems in the solid state using NMR"
- C. Birattari, P. Cappellaro, A. Mitaroff and M. Silari "Development of an Extended Range Bonner Sphere Spectrometer"
2024 | UP ↑ |
PRX Quantum 5, 010321 (2024) |
|
Abstract: Electronic spin defects in the environment of an optically active spin can be used to increase the size and hence the performance of solid-state quantum registers, especially for applications in quantum metrology and quantum communication. Previous works on multiqubit electronic spin registers in the environment of a nitrogen-vacancy (NV) center in diamond have only included spins directly coupled to the NV. As this direct coupling is limited by the central spin coherence time, it significantly restricts the maximum attainable size of the register. To address this problem, we present a scalable approach to increase the size of electronic spin registers. Our approach exploits a weakly coupled probe spin together with double-resonance control sequences to mediate the transfer of spin polarization between the central NV spin and an environmental spin that is not directly coupled to it. We experimentally realize this approach to demonstrate the detection and coherent control of an unknown electronic spin outside the coherence limit of a central NV. Our work paves the way for engineering larger quantum spin registers with the potential to advance nanoscale sensing, enable correlated noise spectroscopy for error correction, and facilitate the realization of spin-chain quantum wires for quantum communication. | |
BibTeX:
@article{Ungar24, author = {Ungar, Alexander and Cappellaro, Paola and Cooper, Alexandre and Sun, Won Kyu Calvin}, title = {Control of an Environmental Spin Defect beyond the Coherence Limit of a Central Spin}, journal = {PRX Quantum}, publisher = {American Physical Society}, year = {2024}, volume = {5}, pages = {010321}, doi = {10.1103/PRXQuantum.5.010321} } |
|
arXiv:2310.19741 (2023) |
|
Abstract: Performing parallel gate operations while retaining low crosstalk is an essential step in transforming neutral atom arrays into powerful quantum computers and simulators. Tightly focusing control beams in small areas for crosstalk suppression is typically challenging and can lead to imperfect polarization for certain transitions. We tackle such a problem by introducing a method to engineer single qubit gates through phase-modulated continuous driving. Distinct qubits can be individually addressed to high accuracy by simply tuning the modulation parameters, which significantly suppresses crosstalk effects. When arranged in a lattice structure, individual control with optimal crosstalk suppression is achieved. With the assistance of additional addressing light or multiple modulation frequencies, we develop two efficient implementations of parallel-gate operations. Our results pave the way to scaling up atom-array platforms with low-error parallel-gate operations, without requiring complicated wavefront design or high-power laser beams. | |
BibTeX:
@article{Wang23x, author = {Guoqing Wang and Wenchao Xu and Changhao Li and Vladan Vuletić and Paola Cappellaro}, title = {Individual-atom control in array through phase modulation}, journal = {arXiv:2310.19741}, year = {2023} } |
|
arXiv:2401.01333 (2024) |
|
Abstract: Nuclear spins in solid-state platforms are promising for building rotation sensors due to their long coherence times. Among these platforms, nitrogen-vacancy centers have attracted considerable attention with ambient operating conditions. However, the current performance of NV gyroscopes remains limited by the degraded coherence when operating with large spin ensembles. Protecting the coherence of these systems requires a systematic study of the coherence decay mechanism. Here we present the use of nitrogen-15 nuclear spins of NV centers in building gyroscopes, benefiting from its simpler energy structure and vanishing nuclear quadrupole term compared with nitrogen-14 nuclear spins, though suffering from different challenges in coherence protection. We systematically reveal the coherence decay mechanism of the nuclear spin in different NV electronic spin manifolds and further develop a robust coherence protection protocol based on controlling the NV electronic spin only, achieving a 15-fold dephasing time improvement. With the developed coherence protection, we demonstrate an emulated gyroscope by measuring a designed rotation rate pattern, showing an order-of-magnitude sensitivity improvement. | |
BibTeX:
@article{Wang24x2, author = {Guoqing Wang and Minh-Thi Nguyen and Dane W. deQuilettes and Eden Price and Zhiyao Hu and Danielle A. Braje and Paola Cappellaro}, title = {Emulated nuclear spin gyroscope with ^15NV centers in diamond}, journal = {arXiv:2401.01333}, year = {2024} } |
|
arXiv:2401.01334 (2024) |
|
Abstract: Solid-state platforms based on electro-nuclear spin systems are attractive candidates for rotation sensing due to their excellent sensitivity, stability, and compact size, compatible with industrial applications. Conventional spin-based gyroscopes measure the accumulated phase of a nuclear spin superposition state to extract the rotation rate and thus suffer from spin dephasing. Here, we propose a gyroscope protocol based on a two-spin system that includes a spin intrinsically tied to the host material, while the other spin is isolated. The rotation rate is then extracted by measuring the relative rotation angle between the two spins starting from their population states, robust against spin dephasing. In particular, the relative rotation rate between the two spins can be enhanced by their hyperfine coupling by more than an order of magnitude, further boosting the achievable sensitivity. The ultimate sensitivity of the gyroscope is limited by the lifetime of the spin system and compatible with a broad dynamic range, even in the presence of magnetic noises or control errors due to initialization and qubit manipulations. Our result enables precise measurement of slow rotations and exploration of fundamental physics. | |
BibTeX:
@article{Wang24x1, author = {Guoqing Wang and Minh-Thi Nguyen and Paola Cappellaro}, title = {Hyperfine-enhanced gyroscope based on solid-state spins}, journal = {arXiv:2401.01334}, year = {2024} } |
|
arXiv:2309.07100 (2023) |
|
Abstract: The nuclear strong force induces the widely studied neutron scattering states and MeV-energy nuclear bound states. Whether this same interaction could lead to low-energy bound states for a neutron in the nuclear force field of a cluster of nuclei is an open question. Here, we computationally demonstrate the existence of -μeV-level neutronic bound states originating from nuclear interaction in nanocrystals with a spatial extent of tens of nanometers. These negative-energy neutron wavefunctions depend on the size, dimension, and nuclear spin polarization of the nanoparticles, providing engineering degrees of freedom for the artificial neutronic "molecule". | |
BibTeX:
@article{Tang23x, author = {Hao Tang and Guoqing Wang and Paola Cappellaro and Ju Li}, title = {μeV-deep neutron bound states in nanocrystals}, journal = {arXiv:2309.07100}, year = {2023} } |
|
arXiv:2309.07731 (2023) |
|
Abstract: Certain non-Hermitian systems exhibit the skin effect, whereby the wavefunctions become exponentially localized at one edge of the system. Such exponential amplification of wavefunction has received significant attention due to its potential applications in e.g., classical and quantum sensing. However, the opposite edge of the system, featured by the exponentially suppressed wavefunctions, remains largely unexplored. Leveraging this phenomenon, we introduce a non-Hermitian cooling mechanism, which is fundamentally distinct from traditional refrigeration or laser cooling techniques. Notably, non-Hermiticity will not amplify thermal excitations, but rather redistribute them. Hence, thermal excitations can be cooled down at one edge of the system, and the cooling effect can be exponentially enhanced by the number of auxiliary modes, albeit with a lower bound that depends on the dissipative interaction with the environment. Non-Hermitian cooling does not rely on intricate properties such as exceptional points or non-trivial topology, and it can apply to a wide range of Bosonic modes such as photons, phonons, magnons, etc. | |
BibTeX:
@article{Xu23x2, author = {Haowei Xu and Uroš Delić and Guoqing Wang and Changhao Li and Paola Cappellaro and Ju Li}, title = {Exponentially Enhanced non-Hermitian Cooling}, journal = {arXiv:2309.07731}, year = {2023} } |
|
ArXiv:2311.16291 (2023) |
|
Abstract: The precise control of complex quantum mechanical systems can unlock applications ranging from quantum simulation to quantum computation. Controlling strongly interacting many-body systems often relies on Floquet Hamiltonian engineering that is achieved by fast switching between Hamiltonian primitives via external control. For example, in our solid-state NMR system, we perform quantum simulation by modulating the natural Hamiltonian with control pulses. As the Floquet heating errors scale with the interpulse delay, δt, it is favorable to keep δt as short as possible, forcing our control pulses to be short duration and high power. Additionally, high-power pulses help to minimize undesirable evolution from occurring during the duration of the pulse. However, such pulses introduce an appreciable phase-transient control error, a form of unitary error. In this work, we detail our ability to diagnose the error, calibrate its magnitude, and correct it for π/2-pulses of arbitrary phase. We demonstrate the improvements gained by correcting for the phase transient error, using a method which we call the ``frame-change technique'', in a variety of experimental settings of interest. Given that the correction mechanism adds no real control overhead, we recommend that any resonance probe be checked for these phase transient control errors, and correct them using the frame-change technique. | |
BibTeX:
@article{Stasiuk23x, author = {Andrew Stasiuk and Pai Peng and Garrett Heller and Paola Cappellaro}, title = {Frame Change Technique for Phase Transient Cancellation}, journal = {ArXiv:2311.16291}, year = {2023} } |
|
ArXiv:2312.08841 (2023) |
|
Abstract: he field of nanoscale magnetic resonance imaging (NanoMRI) was started 30 years ago. It was motivated by the desire to image single molecules and molecular assemblies, such as proteins and virus particles, with near-atomic spatial resolution and on a length scale of 100 nm. Over the years, the NanoMRI field has also expanded to include the goal of useful high-resolution nuclear magnetic resonance (NMR) spectroscopy of molecules under ambient conditions, including samples up to the micron-scale. The realization of these goals requires the development of spin detection techniques that are many orders of magnitude more sensitive than conventional NMR and MRI, capable of detecting and controlling nanoscale ensembles of spins. Over the years, a number of different technical approaches to NanoMRI have emerged, each possessing a distinct set of capabilities for basic and applied areas of science. The goal of this roadmap article is to report the current state of the art in NanoMRI technologies, outline the areas where they are poised to have impact, identify the challenges that lie ahead, and propose methods to meet these challenges. This roadmap also shows how developments in NanoMRI techniques can lead to breakthroughs in emerging quantum science and technology applications. | |
BibTeX:
@article{Budakian23, author = {Raffi Budakian and Amit Finkler and Alexander Eichler and Martino Poggio and Christian L. Degen and Sahand Tabatabaei and Inhee Lee and P. Chris Hammel and Eugene S. Polzik and Tim H. Taminiau and Ronald L. Walsworth and Paz London and Ania Bleszynski Jayich and Ashok Ajoy and Arjun Pillai and Jörg Wrachtrup and Fedor Jelezko and Yujeong Bae and Andreas J. Heinrich and Christian R. Ast and Patrice Bertet and Paola Cappellaro and Cristian Bonato and Yoann Altmann and Erik Gauger}, title = {Roadmap on Nanoscale Magnetic Resonance Imaging}, journal = {Arxiv:2312.08841}, url = {https://arxiv.org/abs/2312.08841}, year = {2023} } |
|
arXiv:2310.12893 (2023) |
|
Abstract: Distributed quantum computing is a promising computational paradigm for performing computations that are beyond the reach of individual quantum devices. Privacy in distributed quantum computing is critical for maintaining confidentiality and protecting the data in the presence of untrusted computing nodes. In this work, we introduce novel blind quantum machine learning protocols based on the quantum bipartite correlator algorithm. Our protocols have reduced communication overhead while preserving the privacy of data from untrusted parties. We introduce robust algorithm-specific privacy-preserving mechanisms with low computational overhead that do not require complex cryptographic techniques. We then validate the effectiveness of the proposed protocols through complexity and privacy analysis. Our findings pave the way for advancements in distributed quantum computing, opening up new possibilities for privacy-aware machine learning applications in the era of quantum technologies. | |
BibTeX:
@article{Li23x2, author = {Changhao Li and Boning Li and Omar Amer and Ruslan Shaydulin and Shouvanik Chakrabarti and Guoqing Wang and Haowei Xu and Hao Tang and Isidor Schoch and Niraj Kumar and Charles Lim and Ju Li and Paola Cappellaro and Marco Pistoia}, title = {Blind quantum machine learning with quantum bipartite correlator}, journal = {arXiv:2310.12893}, year = {2023} } |
|
arXiv:2308.09048 (2023) |
|
Abstract: Transduction of quantum information between distinct quantum systems is an essential step in various applications, including quantum networks and quantum computing. However, mediating photons of vastly different frequencies and designing high-performance transducers are challenging, due to multifaceted and sometimes conflicting requirements. In this work, we first discuss some general principles for quantum transducer design, and then propose solid-state anti-ferromagnetic topological insulators to serve as highly effective transducers. First, topological insulators exhibit band-inversion, which can greatly enhance their optical responses. This property, coupled with robust spin-orbit coupling and high spin density, results in strong nonlinear interaction in magnetic topological insulators, thereby substantially improving transduction efficiency. Second, the anti-ferromagnetic order can minimize the detrimental influence on other neighboring quantum systems due to magnetic interactions. Using MnBi2Te4 as an example, we showcase that single-photon quantum transduction efficiency exceeding 80% can be achieved with modest experimental requirements, while the transduction bandwidth can reach the GHz range. The strong nonlinear photonic interactions in magnetic topological insulators can find diverse applications, including the generation of entanglement between photons of disparate frequencies and quantum squeezing. | |
BibTeX:
@article{Xu23x, author = {Haowei Xu and Changhao Li and Guoqing Wang and Hao Tang and Paola Cappellaro and Ju Li}, title = {Efficient Quantum Transduction Using Anti-Ferromagnetic Topological Insulators}, journal = {arXiv:2308.09048}, year = {2023} } |
|
arXiv:2301.03143 (2023) |
|
Abstract: Alkali metal ions such as sodium and potassium cations play fundamental roles in biology. Developing highly sensitive and selective methods to both detect and quantify these ions is of considerable importance for medical diagnostics and bioimaging. Fluorescent nanoparticles have emerged as powerful tools for nanoscale imaging, but their optical properties need to be supplemented with specificity to particular chemical and biological signals in order to provide further information about biological processes. Nitrogen-vacancy (NV) centers in diamond are particularly attractive as fluorescence markers, thanks to their optical stability, biocompatibility and further ability to serve as highly sensitive quantum sensors of temperature, magnetic and electric fields in ambient conditions. In this work, by covalently grafting crown ether structures on the surface of nanodiamonds (NDs), we build sensors that are capable of detecting specific alkali ions such as sodium cations. We will show that the presence of these metal ions modifies the charge state of NV centers inside the ND, which can then be read out by measuring their photoluminescence spectrum. Our work paves the way for designing selective biosensors based on NV centers in diamond. | |
BibTeX:
@article{Li23x, author = {Li, Changhao and Luo, Shao-Xiong Lennon and Kim, Daniel M. and Wang, Guoqing and Cappellaro, Paola}, title = {Ion sensors with crown ether-functionalized nanodiamonds}, journal = {arXiv:2301.03143}, year = {2023}, doi = {10.48550/ARXIV.2301.03143} } |
|
arXiv:2112.14998 (2022) |
|
Abstract: Quantum sensors can show unprecedented sensitivities, provided they are controlled in a very specific, optimal way. Here, we consider a spin sensor of time-varying fields in the presence of dephasing noise, and we show that the problem of finding the optimal pulsed control field can be mapped to the determination of the ground state of a spin chain. We find an approximate but analytic solution of this problem, which provides a lower bound for the sensor sensitivity, and a pulsed control very close to optimal, which we further use as initial guess for realizing a fast simulated annealing algorithm. We experimentally demonstrate the sensitivity improvement for a spin-qubit magnetometer based on a nitrogen-vacancy center in diamond. | |
BibTeX:
@article{Hernandez22x, author = {Hernández-Gómez, S. and Balducci, F. and Fasiolo, G. and Cappellaro, P. and Fabbri, N. and Scardicchio, A.}, title = {Optimal control of a quantum sensor: A fast algorithm based on an analytic solution}, journal = {arXiv:2112.14998}, year = {2022}, doi = {10.48550/arXiv.2112.14998} } |
|
arXiv:2204.13777 (2022) |
|
Abstract: The power of quantum sensing rests on its ultimate precision limit, quantified by the quantum Cramér-Rao bound (QCRB), which can surpass classical bounds. In multi-parameter estimation, the QCRB is not always saturated as the quantum nature of associated observables may lead to their incompatibility. Here we explore the precision limits of multi-parameter estimation through the lens of quantum geometry, enabling us to experimentally evaluate the QCRB via quantum geometry measurements. Focusing on two- and three-parameter estimation, we elucidate how fundamental quantum uncertainty principles prevent the saturation of the bound. By linking a metric of "quantumness" to the system geometric properties, we investigate and experimentally extract the attainable QCRB for three-parameter estimations. | |
BibTeX:
@article{Li22y, author = {Li, Changhao and Chen, Mo and Cappellaro, Paola}, title = {A geometric perspective: experimental evaluation of the quantum Cramer-Rao bound}, journal = {arXiv:2204.13777}, year = {2022}, doi = {10.48550/arXiv.2204.13777} } |
|
2023 | UP ↑ |
Phys. Rev. X 13, 041016 (2023) |
|
Abstract: A time crystal is a state of periodically driven matter which breaks discrete time translation symmetry. Time crystals have been demonstrated experimentally in various programmable quantum simulators and exemplify how non-equilibrium, driven quantum systems can exhibit intriguing and robust properties absent in systems at equilibrium. These robust driven states need to be stabilized by some mechanism, with the preeminent candidates being many-body localization and prethermalization. This introduces additional constraints that make it challenging to experimentally observe time crystallinity in naturally occurring systems. Recent theoretical work has developed the notion of prethermalization without temperature, expanding the class of time crystal systems to explain time crystalline observations at (or near) infinite temperature. In this work, we conclusively observe the emergence of a prethermal U(1) time crystalline state at quasi-infinite temperature in a solid-state NMR quantum emulator by verifying the requisites of prethermalization without temperature. In addition to observing the signature period-doubling behavior, we show the existence of a long-lived prethermal regime whose lifetime is significantly enhanced by strengthening an emergent U(1) conservation law. Not only do we measure this enhancement through the global magnetization, but we also exploit on-site disorder to measure local observables, ruling out the possibility of many-body localization and confirming the emergence of long-range correlations. | |
BibTeX:
@article{Stasiuk23, author = {Stasiuk, Andrew and Cappellaro, Paola}, title = {Observation of a Prethermal U(1) Discrete Time Crystal}, journal = {Phys. Rev. X}, publisher = {American Physical Society}, year = {2023}, volume = {13}, pages = {041016}, doi = {10.1103/PhysRevX.13.041016} } |
|
Phys. Rev. A 107, 062412 (2023) |
|
Abstract: The Vlasov equation is a nonlinear partial differential equation that provides a first-principles description of the dynamics of plasmas. Its linear limit is routinely used in plasma physics to investigate plasma oscillations and stability. In this paper, we present a quantum algorithm that simulates the linearized Vlasov equation with and without collisions, in the one-dimensional electrostatic limit. Rather than solving this equation in its native spatial and velocity phase space, we adopt an efficient representation in the dual space yielded by a Fourier-Hermite expansion. For a given simulation time, the Fourier-Hermite representation is exponentially more compact, thus yielding a classical algorithm that can match the performance of a previously proposed quantum algorithm for this problem. This representation results in a system of linear ordinary differential equations (ODEs) which can be solved with well-developed quantum algorithms: a Hamiltonian simulation in the collisionless case, and quantum ODE solvers in the collisional case. In particular, we demonstrate that a quadratic speedup in system size is attainable. | |
BibTeX:
@article{Ameri23, author = {Ameri, Abtin and Ye, Erika and Cappellaro, Paola and Krovi, Hari and Loureiro, Nuno F.}, title = {Quantum algorithm for the linear Vlasov equation with collisions}, journal = {Phys. Rev. A}, year = {2023}, volume = {107}, pages = {062412}, doi = {10.1103/PhysRevA.107.062412} } |
|
Phys. Rev. Lett. 131, 043602 (2023) |
|
Abstract: Solid-state spin defects, especially nuclear spins with potentially achievable long coherence times, are compelling candidates for quantum memories and sensors. However, their current performances are still limited by dephasing due to variations of their intrinsic quadrupole and hyperfine interactions. We propose an unbalanced echo to overcome this challenge by using a second spin to refocus variations of these interactions while preserving the quantum information stored in the nuclear spin free evolution. The unbalanced echo can be used to probe the temperature and strain distribution in materials. We develop first-principles methods to predict variations of these interactions and reveal their correlation over large temperature and strain ranges. Experiments performed in an ensemble of ∼ 10 10 nuclear spins in diamond demonstrate a 20-fold dephasing time increase, limited by other noise sources. We further numerically show that our method can refocus even stronger noise variations than present in our experiments. |
|
BibTeX:
@article{Wang23, author = {Wang, Guoqing and Barr, Ariel Rebekah and Tang, Hao and Chen, Mo and Li, Changhao and Xu, Haowei and Stasiuk, Andrew and Li, Ju and Cappellaro, Paola}, title = {Characterizing Temperature and Strain Variations with Qubit Ensembles for Their Robust Coherence Protection}, journal = {Phys. Rev. Lett.}, publisher = {American Physical Society}, year = {2023}, volume = {131}, pages = {043602}, doi = {10.1103/PhysRevLett.131.043602} } |
|
The Journal of Physical Chemistry Letters 14, 3266-3273 (2023) |
|
Abstract: Spin qubits associated with color centers are promising platforms for various quantum technologies. However, to be deployed in robust quantum devices, the variations of their intrinsic properties with the external conditions, in particular temperature and strain, should be known with high precision. Unfortunately, a predictive theory on the temperature dependence of the resonance frequency of electron and nuclear spin defects in solids remains lacking. In this work, we develop a first-principles method for the temperature dependence of the zero-field splitting, hyperfine interaction, and nuclear quadrupole interaction of color centers. As a testbed, we compare our ab initio calculations with experiments for the nitrogen-vacancy (NV–) center in diamond, finding good agreements. We identify the major origin of the temperature dependence as a second-order effect of dynamic phonon vibrations, instead of the thermal-expansion strain. The method can be applied to different color centers and provides a theoretical tool for designing high-precision quantum sensors. | |
BibTeX:
@article{Tang23a, author = {Tang, Hao and Barr, Ariel Rebekah and Wang, Guoqing and Cappellaro, Paola and Li, Ju}, title = {First-Principles Calculation of the Temperature-Dependent Transition Energies in Spin Defects}, journal = {The Journal of Physical Chemistry Letters}, year = {2023}, volume = {14}, number = {13}, pages = {3266-3273}, doi = {10.1021/acs.jpclett.3c00314} } |
|
Proc. Nat. Acad. Sc. 120, e2305621120 (2023) |
|
Abstract: Solid-state defects are attractive platforms for quantum sensing and simulation, e.g., in exploring many-body physics and quantum hydrodynamics. However, many interesting properties can be revealed only upon changes in the density of defects, which instead is usually fixed in material systems. Increasing the interaction strength by creating denser defect ensembles also brings more decoherence. Ideally one would like to control the spin concentration at will while keeping fixed decoherence effects. Here, we show that by exploiting charge transport, we can take some steps in this direction, while at the same time characterizing charge transport and its capture by defects. By exploiting the cycling process of ionization and recombination of NV centers in diamond, we pump electrons from the valence band to the conduction band. These charges are then transported to modulate the spin concentration by changing the charge state of material defects. By developing a wide-field imaging setup integrated with a fast single photon detector array, we achieve a direct and efficient characterization of the charge redistribution process by measuring the complete spectrum of the spin bath with micrometer-scale spatial resolution. We demonstrate a two-fold concentration increase of the dominant spin defects while keeping the T2 of the NV center relatively unchanged, which also provides a potential experimental demonstration of the suppression of spin flip-flops via hyperfine interactions. Our work paves the way to studying many-body dynamics with temporally and spatially tunable interaction strengths in hybrid charge–spin systems. | |
BibTeX:
@article{Wang23p, author = {Guoqing Wang and Changhao Li and Hao Tang and Boning Li and Francesca Madonini and Faisal F. Alsallom and Won Kyu Calvin Sun and Pai Peng and Federica Villa and Ju Li and Paola Cappellaro}, title = {Manipulating solid-state spin concentration through charge transport}, journal = {Proc. Nat. Acad. Sc.}, year = {2023}, volume = {120}, number = {32}, pages = {e2305621120}, doi = {10.1073/pnas.2305621120} } |
|
Phys. Rev. Lett. 130, 150602 (2023) |
|
Abstract: The growing demands of remote detection and an increasing amount of training data make distributed machine learning under communication constraints a critical issue. This work provides a communication-efficient quantum algorithm that tackles two traditional machine learning problems, the least-square fitting and softmax regression problems, in the scenario where the dataset is distributed across two parties. Our quantum algorithm finds the model parameters with a communication complexity of O(log2(N)/ε), where N is the number of data points and ε is the bound on parameter errors. Compared to classical and other quantum methods that achieve the same goal, our methods provide a communication advantage in the scaling with data volume. The core of our methods, the quantum bipartite correlator algorithm that estimates the correlation or the Hamming distance of two bit strings distributed across two parties, may be further applied to other information processing tasks. |
|
BibTeX:
@article{Hao23l, author = {Tang, Hao and Li, Boning and Wang, Guoqing and Xu, Haowei and Li, Changhao and Barr, Ariel and Cappellaro, Paola and Li, Ju}, title = {Communication-Efficient Quantum Algorithm for Distributed Machine Learning}, journal = {Phys. Rev. Lett.}, publisher = {American Physical Society}, year = {2023}, volume = {130}, pages = {150602}, doi = {10.1103/PhysRevLett.130.150602} } |
|
Phys. Rev. A 108, L021502 (2023) |
|
Abstract: The radiative excitation of the 8.3 eV isomeric state of 229Th is an long-standing challenge due to the lack of tunable far-ultraviolet (FUV) sources. In this work, we propose an efficient two-photon pumping scheme for 229 Th using the optonuclear quadrupolar effect, which only requires a 300 nm UV-B pumping laser. We further demonstrate that population inversion between the nuclear isomeric and ground states can be achieved at room temperature using a two-step pumping process. The nuclear laser, which has been pursued unsuccessfully for decades, may be realized using a watt-level UV-B pumping laser and ultrawide band gap thorium compounds (e.g., ThF4, Na2ThF6 or K2ThF6) as the gain medium. |
|
BibTeX:
@article{Xu23a, author = {Xu, Haowei and Tang, Hao and Wang, Guoqing and Li, Changhao and Li, Boning and Cappellaro, Paola and Li, Ju}, title = {Solid-state ^229Th nuclear laser with two-photon pumping}, journal = {Phys. Rev. A}, publisher = {American Physical Society}, year = {2023}, volume = {108}, pages = {L021502}, doi = {10.1103/PhysRevA.108.L021502} } |
|
Adv Quantum Technol. (2023) |
|
Abstract: Achieving fast, sensitive, and parallel measurement of a large number of quantum particles is an essential task in building large-scale quantum platforms for different quantum information processing applications such as sensing, computation, simulation, and communication. Current quantum platforms in experimental atomic and optical physics based on CMOS sensors and CCD cameras are limited by either low sensitivity or slow operational speed. Here we integrate an array of single-photon avalanche diodes with solid-state spin defects in diamond to build a fast wide-field quantum sensor, achieving a frame rate up to 100textasciitilde kHz. We present the design of the experimental setup to perform spatially resolved imaging of quantum systems. A few exemplary applications, including sensing DC and AC magnetic fields, temperature, strain, local spin density, and charge dynamics, are experimentally demonstrated using an NV ensemble diamond sample. The developed photon detection array is broadly applicable to other platforms such as atom arrays trapped in optical tweezers, optical lattices, donors in silicon, and rare earth ions in solids. | |
BibTeX:
@article{Wang23s, author = {Wang, Guoqing and Madonini, Francesca and Li, Boning and Li, Changhao and Xiang, Jinggang and Villa, Federica and Cappellaro, Paola}, title = {Fast Wide-Field Quantum Sensor Based on Solid-State Spins Integrated with a SPAD Array}, journal = {Adv Quantum Technol.}, year = {2023}, doi = {10.1002/qute.202300046} } |
|
Nature Physics (2023) |
|
Abstract: An outstanding challenge in large-scale quantum platforms is to simultaneously achieve strong interactions, giving rise to the most interesting behaviors, and local addressing -that can probe them. In the context of correlated phases, local addressing enables one to directly probe the nature of the system's order. Meanwhile, for out-ofequilibrium dynamics, such addressing allows the study of quantum information spreading and operator growth. Here, we introduce a novel technique that enables the measurement of local correlation functions, down to single-site resolution, despite access to only global controls. Our approach leverages the intrinsic disorder present in a solid-state spin ensemble to dephase the nonlocal components of the correlation function. Utilizing this toolset, we measure both the spin and energy transport in nuclear spin chains. By tuning the interaction Hamiltonian via Floquet engineering, we investigate the cross-over between ballistic and diffusive hydrodynamics. Interestingly, when the system is both interacting and (nearly-)integrable, we observe the coexistence of diffusive spin transport with ballistic energy transport. | |
BibTeX:
@article{Peng23, author = {Peng, Pai and Ye, Bingtian and Yao, Norman Y. , and Cappellaro, Paola}, title = {Exploiting disorder to probe spin and energy hydrodynamics}, journal = {Nature Physics}, year = {2023}, doi = {10.1038/s41567-023-02051-1} } |
|
Phys. Rev. X 13, 011017 (2023) |
|
Abstract: Photons and nuclear spins are two well-known building blocks in quantum information science and technology. Establishing an efficient interface between optical photons and nuclear spins, while highly desirable for hybridizing these two quantum systems, is challenging, because the interactions between nuclear spins and the environment are usually weak in magnitude, and there is also a formidable gap between nuclear spin frequencies and optical frequencies. In this work, we propose an optonuclear quadrupolar (ONQ) effect, whereby optical photons can be efficiently coupled to nuclear spins, similar to Raman scattering. Compared to previous works, ancilla electron spins are not required for the ONQ effect. This leads to advantages such as applicability in defect-free nonmagnetic crystals and longer nuclear spin coherence time. In addition, the frequency of the optical photons can be arbitrary, so they can be fine-tuned to minimize the material heating and to match telecom wavelengths for long-distance communications. Using perturbation theory and first-principles calculations, we demonstrate that the ONQ effect is stronger by several orders of magnitude than other nonlinear optical effects that could couple to nuclear spins. Based on this rationale, we propose promising applications of the ONQ effect, including quantum memory, quantum transduction, and materials isotope spectroscopy. We also discuss issues relevant to the experimental demonstration of the ONQ effect. | |
BibTeX:
@article{Xu23, author = {Xu, Haowei and Li, Changhao and Wang, Guoqing and Wang, Hua and Tang, Hao and Barr, Ariel Rebekah and Cappellaro, Paola and Li, Ju}, title = {Two-Photon Interface of Nuclear Spins Based on the Optonuclear Quadrupolar Effect}, journal = {Phys. Rev. X}, publisher = {American Physical Society}, year = {2023}, volume = {13}, pages = {011017}, doi = {10.1103/PhysRevX.13.011017} } |
|
Phys. Rev. Lett. 130, 063602 (2023) |
|
Abstract: The initialization of nuclear spin to its ground state is challenging due to its small energy scale compared with thermal energy, even at cryogenic temperature. In this Letter, we propose an optonuclear quadrupolar effect, whereby two-color optical photons can efficiently interact with nuclear spins. Leveraging such an optical interface, we demonstrate that nuclear magnons, the collective excitations of nuclear spin ensemble, can be cooled down optically. Under feasible experimental conditions, laser cooling can suppress the population and entropy of nuclear magnons by more than 2 orders of magnitude, which could facilitate the application of nuclear spins in quantum information science. | |
BibTeX:
@article{Xu23l, author = {Xu, Haowei and Wang, Guoqing and Li, Changhao and Wang, Hua and Tang, Hao and Barr, Ariel Rebekah and Cappellaro, Paola and Li, Ju}, title = {Laser Cooling of Nuclear Magnons}, journal = {Phys. Rev. Lett.}, publisher = {American Physical Society}, year = {2023}, volume = {130}, pages = {063602}, doi = {10.1103/PhysRevLett.130.063602} } |
|
2022 | UP ↑ |
Science 375, 1017-1020 (2022) |
|
Abstract: Magnetic monopoles play a central role in areas of physics that range from electromagnetism to topological matter. String theory promotes conventional vector gauge fields of electrodynamics to tensor gauge fields and predicts the existence of more exotic tensor monopoles. Here, we report the synthesis of a tensor monopole in a four-dimensional parameter space defined by the spin degrees of freedom of a single solid-state defect in diamond. Using two complementary methods, we characterized the tensor monopole by measuring its quantized topological charge and its emanating Kalb-Ramond field. By introducing a fictitious external field that breaks chiral symmetry, we further observed an intriguing spectral transition, characterized by spectral rings protected by mirror symmetries. Our work demonstrates the possibility of emulating exotic topological structures inspired by string theory. Magnetic monopoles, hypothetical sources of magnetic field in three-dimensional space, have not been observed as elementary particles. However, synthetic monopoles can be engineered in ultracold systems. Going a step further, Chen et al. used the quantum levels of a nitrogen vacancy center in diamond to observe the effects of a synthetic tensor monopole: the generalization of the magnetic monopole to four dimensions. The researchers modulated an applied microwave pulse to measure the “magnetic” field emanating from the tensor monopole and its topological charge. —JS The three-level system in a diamond nitrogen vacancy center is used to engineer a tensor monopole. | |
BibTeX:
@article{Chen22, author = {Mo Chen and Changhao Li and Giandomenico Palumbo and Yan-Qing Zhu and Nathan Goldman and Paola Cappellaro}, title = {A synthetic monopole source of Kalb-Ramond field in diamond}, journal = {Science}, year = {2022}, volume = {375}, number = {6584}, pages = {1017-1020}, doi = {10.1126/science.abe6437} } |
|
Phys. Rev. X 12, 021061 (2022) |
|
Abstract: Quantum sensors such as spin defects in diamond have achieved excellent performance by combining high sensitivity with spatial resolution. Unfortunately, these sensors can only detect signal fields with frequency in a few accessible ranges, typically low frequencies up to the experimentally achievable control field amplitudes and a narrow window around the sensors’ resonance frequency. Here, we develop and demonstrate a technique for sensing arbitrary-frequency signals by using the sensor qubit as a quantum frequency mixer, enabling a variety of sensing applications. The technique leverages nonlinear effects in periodically driven (Floquet) quantum systems to achieve quantum frequency mixing of the signal and an applied bias ac field. The frequency-mixed field can be detected using well-developed sensing techniques such as Rabi and CPMG with the only additional requirement of the bias field. We further show that the frequency mixing can distinguish vectorial components of an oscillating signal field, thus enabling arbitrary-frequency vector magnetometry. We experimentally demonstrate this protocol with nitrogen-vacancy centers in diamond to sense a 150-MHz signal field, proving the versatility of the quantum mixer sensing technique. | |
BibTeX:
@article{Wang22, author = {Wang, Guoqing and Liu, Yi-Xiang and Schloss, Jennifer M. and Alsid, Scott T. and Braje, Danielle A. and Cappellaro, Paola}, title = {Sensing of Arbitrary-Frequency Fields Using a Quantum Mixer}, journal = {Phys. Rev. X}, publisher = {American Physical Society}, year = {2022}, volume = {12}, pages = {021061}, doi = {10.1103/PhysRevX.12.021061} } |
|
Phys. Rev. Lett. 128, 140503 (2022) |
|
Abstract: The sensitivity afforded by quantum sensors is limited by decoherence. Quantum error correction (QEC) can enhance sensitivity by suppressing decoherence, but it has a side effect: it biases a sensor’s output in realistic settings. If unaccounted for, this bias can systematically reduce a sensor’s performance in experiment, and also give misleading values for the minimum detectable signal in theory. We analyze this effect in the experimentally motivated setting of continuous-time QEC, showing both how one can remedy it, and how incorrect results can arise when one does not. | |
BibTeX:
@article{Rojkov21, author = {Rojkov, Ivan and Layden, David and Cappellaro, Paola and Home, Jonathan and Reiter, Florentin}, title = {Bias in Error-Corrected Quantum Sensing}, journal = {Phys. Rev. Lett.}, year = {2022}, volume = {128}, pages = {140503}, doi = {10.1103/PhysRevLett.128.140503} } |
|
PRX Quantum 3, 020329 (2022) |
|
Abstract: Engineered dynamical maps combining coherent and dissipative transformations of quantum states with quantum measurements have demonstrated a number of technological applications, and promise to be a crucial tool in quantum thermodynamic processes. Here we exploit the control on the effective open spin qutrit dynamics of a nitrogen-vacancy center to experimentally realize an autonomous feedback process (Maxwell’s demon) with tunable dissipative strength. The feedback is enabled by random measurement events that condition the subsequent dissipative evolution of the qutrit. The efficacy of the autonomous Maxwell's demon is quantified by means of a generalized Sagawa-Ueda-Tasaki relation for dissipative dynamics. To achieve this, we experimentally characterize the fluctuations of the energy exchanged between the system and its the environment. This opens the way to the implementation of a new class of Maxwell’s demons, which could be useful for quantum sensing and quantum thermodynamic devices. | |
BibTeX:
@article{Hernandez22, author = {Hernández-Gómez, S. and Gherardini, S. and Staudenmaier, N. and Poggiali, F. and Campisi, M. and Trombettoni, A. and Cataliotti, F.S. and Cappellaro, P. and Fabbri, N.}, title = {Autonomous Dissipative Maxwell's Demon in a Diamond Spin Qutrit}, journal = {PRX Quantum}, publisher = {American Physical Society}, year = {2022}, volume = {3}, pages = {020329}, doi = {10.1103/PRXQuantum.3.020329} } |
|
Phys. Rev. Applied 18, 024033 (2022) |
|
Abstract: Engineering desired Hamiltonians in quantum many-body systems is essential for applications such as quantum simulation, computation, and sensing. Many widely used quantum Hamiltonian engineering sequences are designed using human intuition based on perturbation theory, which may not describe the optimal solution and is unable to accommodate complex experimental imperfections. Here we numerically search for Hamiltonian engineering sequences using deep reinforcement learning (DRL) techniques and experimentally demonstrate that they outperform celebrated decoupling sequences on a solid-state nuclear magnetic resonance quantum simulator. As an example, we aim at decoupling strongly interacting spin-1/2 systems. We train DRL agents in the presence of different experimental imperfections and verify robustness of the output sequences both in simulations and experiments. Surprisingly, many of the learned sequences exhibit a common pattern that had not been discovered before, to our knowledge, but has a meaningful analytical description. We can thus restrict the searching space based on this control pattern, allowing us to search for longer sequences, ultimately leading to sequences that are robust against dominant imperfections in our experiments. Our results not only demonstrate a general method for quantum Hamiltonian engineering, but also highlight the importance of combining black-box artificial intelligence with an understanding of the physical system in order to realize experimentally feasible applications. | |
BibTeX:
@article{Pai22, author = {Peng, Pai and Huang, Xiaoyang and Yin, Chao and Joseph, Linta and Ramanathan, Chandrasekhar and Cappellaro, Paola}, title = {Deep Reinforcement Learning for Quantum Hamiltonian Engineering}, journal = {Phys. Rev. Applied}, publisher = {American Physical Society}, year = {2022}, volume = {18}, pages = {024033}, doi = {10.1103/PhysRevApplied.18.024033} } |
|
Phys. Rev. B 106, 155413 (2022) |
|
Abstract: Characterizing and understanding the environment affecting quantum systems is critical to elucidate its physical properties and engineer better quantum devices. We develop an approach to reduce the quantum environment causing single-qubit dephasing to a simple yet predictive noise model. Our approach, inspired by quantum noise spectroscopy, is to define a “self-consistent” classical noise spectrum, that is, compatible with all observed decoherence under various qubit dynamics. We demonstrate the power and limits of our approach by characterizing, with nanoscale spatial resolution, the noise experienced by two electronic spins in diamond that, despite their proximity, surprisingly reveal the presence of a complex quantum spin environment, both classically reducible and not. Our results overcome the limitations of existing noise spectroscopy methods and highlight the importance of finding predictive models to accurately characterize the underlying environment. Extending our work to multiqubit systems would enable spatially resolved quantum sensing of complex environments and quantum device characterization, notably to identify correlated noise between qubits, which is crucial for practical realization of quantum error correction. | |
BibTeX:
@article{Sun22, author = {Sun, Won Kyu Calvin and Cappellaro, Paola}, title = {Self-consistent noise characterization of quantum devices}, journal = {Phys. Rev. B}, publisher = {American Physical Society}, year = {2022}, volume = {106}, pages = {155413}, doi = {10.1103/PhysRevB.106.155413} } |
|
2021 | UP ↑ |
Nano Lett. 21(2021) |
|
Abstract: The development of highly sensitive and rapid biosensing tools targeted to the highly contagious virus SARS-CoV-2 is critical to tackling the COVID-19 pandemic. Quantum sensors can play an important role because of their superior sensitivity and fast improvements in recent years. Here we propose a molecular transducer designed for nitrogen-vacancy (NV) centers in nanodiamonds, translating the presence of SARS-CoV-2 RNA into an unambiguous magnetic noise signal that can be optically read out. We evaluate the performance of the hybrid sensor, including its sensitivity and false negative rate, and compare it to widespread diagnostic methods. The proposed method is fast and promises to reach a sensitivity down to a few hundreds of RNA copies with false negative rate less than 1%. The proposed hybrid sensor can be further implemented with different solid-state defects and substrates, generalized to diagnose other RNA viruses, and integrated with CRISPR technology. | |
BibTeX:
@article{Li21n, author = {Li, Changhao and Soleyman, Rouhollah and Kohandel, Mohammad and Cappellaro, Paola}, title = {SARS-CoV-2 Quantum Sensor Based on Nitrogen-Vacancy Centers in Diamond}, journal = {Nano Lett.}, publisher = {American Chemical Society}, year = {2021}, volume = {21}, number = {12}, pages = {5143--5150}, doi = {10.1021/acs.nanolett.1c02868} } |
|
Nano Lett. 21, 5143-5150 (2021) |
|
Abstract: Detection of AC magnetic fields at the nanoscale is critical in applications ranging from fundamental physics to materials science. Isolated quantum spin defects, such as the nitrogen-vacancy center in diamond, can achieve the desired spatial resolution with high sensitivity. Still, vector AC magnetometry currently relies on using different orientations of an ensemble of sensors, with degraded spatial resolution, and a protocol based on a single NV is lacking. Here we propose and experimentally demonstrate a protocol that exploits a single NV to reconstruct the vectorial components of an AC magnetic field by tuning a continuous driving to distinct resonance conditions. We map the spatial distribution of an AC field generated by a copper wire on the surface of the diamond. The proposed protocol combines high sensitivity, broad dynamic range, and sensitivity to both coherent and stochastic signals, with broad applications in condensed matter physics, such as probing spin fluctuations. | |
BibTeX
@article{Wang21, author = {Wang, Guoqing and Liu, Yi-Xiang and Zhu, Yuan and Cappellaro, Paola}, title = {Nanoscale Vector AC Magnetometry with a Single Nitrogen-Vacancy Center in Diamond}, journal = {Nano Lett.}, publisher = {American Chemical Society}, year = {2021}, volume = {21}, number = {12}, pages = {5143--5150}, doi = {10.1021/acs.nanolett.1c01165} } |
|
Phys. Rev. Lett.127, 140604 (2021) |
|
Abstract: Periodically driven quantum systems, known as Floquet systems, have been a focus of non-equilibrium physics in recent years, thanks to their rich dynamics. Not only time-periodic systems exhibit symmetries similar to those in spatially periodic systems, but they also display novel behavior due to symmetry breaking. Characterizing such dynamical symmetries is crucial, but the task is often challenging, due to limited driving strength and the lack of an experimentally accessible characterization protocol. Here, we show how to characterize dynamical symmetries including parity, rotation, and particle-hole symmetry by observing the symmetry-induced selection rules between Floquet states. Specifically, we exploit modulated quantum driving to reach the strong light-matter coupling regime and we introduce a protocol to experimentally extract the transition elements between Floquet states from the coherent evolution of the system. Using the nitrogen-vacancy center in diamond as an experimental testbed, we apply our methods to observe symmetry-protected dark states and dark bands, and the coherent destruction of tunneling effect. Our work shows how to exploit the quantum control toolkit to study dynamical symmetries that can arise in topological phases of strongly-driven Floquet systems. | |
BibTeX:
@article{Wang21l, author = {Guoqing Wang and Changhao Li and Paola Cappellaro}, title = {Observation of symmetry-protected selection rules in periodically driven quantum systems}, journal = {Phys. Rev. Lett}, volume = {127}, pages = {140604}, doi = {https://doi.org/10.1103/PhysRevLett.127.140604}, year = {2021} } |
|
Nat. Phys. , s41567 (2021) |
|
Abstract: Periodically driven Floquet quantum systems could provide a promising platform to investigate novel physics out of equilibrium1, but the drive generically heats the system to a featureless infinite-temperature state2-4. Fortunately, for high driving frequency, the heat absorption rate has been theoretically predicted to be exponentially small, giving rise to a long-lived prethermal regime that exhibits all the intriguing properties of Floquet systems5-8. Here we experimentally observe Floquet prethermalization using NMR techniques and probe the heating rate. We first show the relaxation of a far-from-equilibrium initial state to a long-lived prethermal state, well described by a time-independent ‘prethermal’ Hamiltonian. By measuring the autocorrelation of this prethermal Hamiltonian we can further experimentally confirm the predicted exponentially slow heating rate. More strikingly, we find that, on the timescale at which the prethermal Hamiltonian picture breaks down, the Floquet system still possesses other quasiconservation laws. Our results demonstrate that it is possible to realize robust Floquet engineering, thus enabling the experimental observation of non-trivial Floquet phases of matter. | |
BibTeX:
@article{Peng21, author = {Peng, Pai and Yin, Chao and Huang, Xiaoyang and Ramanathan, Chandrasekhar and Cappellaro, Paola}, title = {Floquet prethermalization in dipolar spin chains}, journal = {Nat. Phys.}, year = {2021}, pages = {s41567}, doi = {10.1038/s41567-020-01120-z} } |
|
npj Q. Inf. 7, 10 (2021) |
|
Abstract: Quantum network is a promising platform for many ground-breaking applications that lie beyond the capability of its classical counterparts. Efficient entanglement generation on quantum networks with relatively limited resources such as quantum memories is essential to fully realize the network’s capabilities, the solution to which calls for delicate network design and is currently at the primitive stage. In this study we propose an effective routing scheme to enable automatic responses for multiple requests of entanglement generation between source-terminal stations on a quantum lattice network with finite edge capacities. Multiple connection paths are exploited for each connection request while entanglement fidelity is ensured for each path by performing entanglement purification. The routing scheme is highly modularized with a flexible nature, embedding quantum operations within the algorithmic workflow, whose performance is evaluated from multiple perspectives. In particular, three algorithms are proposed and compared for the scheduling of capacity allocation on the edges of quantum network. Embodying the ideas of proportional share and progressive filling that have been well-studied in classical routing problems, we design another scheduling algorithm, the propagatory update method, which in certain aspects overrides the two algorithms based on classical heuristics in scheduling performances. The general solution scheme paves the road for effective design of efficient routing and flow control protocols on applicational quantum networks. | |
BibTeX:
@article{Li21, author = {Li, Changhao and Li, Tianyi and Liu, Yi-Xiang and Cappellaro, Paola}, title = {Effective routing design for remote entanglement generation on quantum networks}, journal = {npj Q. Inf.}, year = {2021}, volume = {7}, number = {1}, pages = {10}, doi = {10.1038/s41534-020-00344-4} } |
|
Phys. Rev. A 103, 022415 (2021) |
|
Abstract: The Mollow triplet is a fundamental signature of quantum optics and has been observed in numerous quantum systems. Although it arises in the “strong driving” regime of the quantized field, where the atoms undergo coherent oscillations, it can be typically analyzed within the rotating wave approximation. Here we report the first observation of high-order effects in the Mollow triplet structure due to strong driving. In experiments, we explore the regime beyond the rotating wave approximation using concatenated continuous driving that has less stringent requirements on the driving field power. We are then able to reveal additional transition frequencies, shifts in energy levels, and corrections to the transition amplitudes. In particular, we find that these amplitudes are more sensitive to high-order effects than the frequency shifts and that they still require an accurate determination in order to achieve high-fidelity quantum control. The experimental results are validated by Floquet theory, which enables the precise numerical simulation of the evolution and further provides an analytical form for an effective Hamiltonian that approximately predicts the spin dynamics beyond the rotating wave approximation. | |
BibTeX:
@article{Wang21a, author = {Wang, Guoqing and Liu, Yi-Xiang and Cappellaro, Paola}, title = {Observation of the high-order Mollow triplet by quantum mode control with concatenated continuous driving}, journal = {Phys. Rev. A}, publisher = {American Physical Society}, year = {2021}, volume = {103}, pages = {022415}, doi = {10.1103/PhysRevA.103.022415} } |
|
Phys. Rev. B 103, 054305 (2021) |
|
Abstract: Prethermalization, by introducing emergent quasiconserved observables, plays a crucial role in protecting periodically driven (Floquet) many-body phases over an exponentially long time, while the ultimate fate of such quasiconserved operators can signal thermalization to infinite temperature. To elucidate the properties of prethermal quasiconservation in many-body Floquet systems, here we systematically analyze infinite-temperature correlations between observables. We numerically show that the late-time behavior of the autocorrelations unambiguously distinguishes quasiconserved observables from nonconserved ones, allowing one to single out a set of linearly independent quasiconserved observables. By investigating two Floquet spin models, we identify two different mechanisms underlying the quasiconservation law. First, we numerically verify energy quasiconservation when the driving frequency is large, so that the system dynamics is approximately described by a static prethermal Hamiltonian. More interestingly, under moderate driving frequency, another quasiconserved observable can still persist if the Floquet driving contains a large global rotation. We show theoretically how to calculate this conserved observable and provide numerical verification. Having systematically identified all quasiconserved observables, we can finally investigate their behavior in the infinite-time limit and thermodynamic limit, using autocorrelations obtained from both numerical simulation and experiments in solid-state nuclear magnetic resonance systems. | |
BibTeX:
@article{Yin21, author = {Yin, Chao and Peng, Pai and Huang, Xiaoyang and Ramanathan, Chandrasekhar and Cappellaro, Paola}, title = {Prethermal quasiconserved observables in Floquet quantum systems}, journal = {Phys. Rev. B}, publisher = {American Physical Society}, year = {2021}, volume = {103}, pages = {054305}, doi = {10.1103/PhysRevB.103.054305} } |
|
2020 | UP ↑ |
New J. Phys. 22, 123045 (2020) |
|
Abstract: Dense ensembles of spin qubits are valuable for quantum applications, even though their coherence protection remains challenging. Continuous dynamical decoupling can protect ensemble qubits from noise while allowing gate operations, but it is hindered by the additional noise introduced by the driving. Concatenated continuous driving (CCD) techniques can, in principle, mitigate this problem. Here we provide deeper insights into the dynamics under CCD, based on Floquet theory, that lead to optimized state protection by adjusting driving parameters in the CCD scheme to induce mode evolution control. We experimentally demonstrate the improved control by simultaneously addressing a dense nitrogen-vacancy (NV) ensemble with 1010 spins. We achieve an experimental 15-fold improvement in coherence time for an arbitrary, unknown state, and a 500-fold improvement for an arbitrary, known state, corresponding to driving the sidebands and the center band of the resulting Mollow triplet, respectively. We can achieve such coherence time gains by optimizing the driving parameters to take into account the noise affecting our system. By extending the generalized Bloch equation approach to the CCD scenario, we identify the noise sources that dominate the decay mechanisms in NV ensembles, confirm our model by experimental results, and identify the driving strengths yielding optimal coherence. Our results can be directly used to optimize qubit coherence protection under continuous driving and bath driving, and enable applications in robust pulse design and quantum sensing. | |
BibTeX:
@article{Wang20n, author = {Wang, Guoqing and Liu, Yi-Xiang and Cappellaro, Paola}, title = {Coherence protection and decay mechanism in qubit ensembles under concatenated continuous driving}, journal = {New J. Phys.}, publisher = {IOP Publishing}, year = {2020}, volume = {22}, number = {12}, pages = {123045}, doi = {10.1088/1367-2630/abd2e5} } |
|
Phys. Rev. Lett. 125, 060602 (2020) |
|
Abstract: In open quantum systems, a clear distinction between work and heat is often challenging, and extending the quantum Jarzynski equality to systems evolving under general quantum channels beyond unitality remains an open problem in quantum thermodynamics. In this letter, we introduce well-defined notions of guessed heat and guessed work, by exploiting the one-time measurement scheme, which only requires an initial energy measurement on the system alone. We derive a modified quantum Jarzynski equality and the principle of maximum work with respect to the guessed quantum work, which requires the knowledge of the system only. We further show the significance of guessed quantum heat and work by linking them to the problem of quantum hypothesis testing. | |
BibTeX:
@article{Sone20, author = {Sone, Akira and Liu, Yi-Xiang and Cappellaro, Paola}, title = {Quantum Jarzynski Equality in Open Quantum Systems from the One-Time Measurement Scheme}, journal = {Phys. Rev. Lett.}, year = {2020}, volume = {125}, pages = {060602}, doi = {10.1103/PhysRevLett.125.060602} } |
|
Phys. Rev. Research 2, 023327 (2020) |
|
Abstract: Elucidating the energy transfer between a quantum system and a reservoir is a central issue in quantum non-equilibrium thermodynamics, which could provide novel tools to engineer quantum-enhanced heat engines. The lack of information on the reservoir inherently limits the practical insight that can be gained on the exchange process. Here, we investigate the energy transfer for an open quantum system in the framework of quantum fluctuation relations. As a novel toolbox, we employ a nitrogen-vacancy center spin qubit in diamond, subject to repeated quantum projective measurements accompanied by a tunable dissipation channel. When the system is tuned to be insensitive to dissipation, we verify the closed-system quantum Jarzynski equality. In the presence of competition between dissipation and quantum projective measurements, the experimental results suggest a formulation of the energy exchange fluctuation relation that incorporates the reservoir properties in the guise of an effective temperature of the final out-of-equilibrium steady-state. Our findings pave the way to investigate energy exchange mechanisms in higher-dimension open quantum systems. | |
BibTeX:
@article{Hernandez20, author = {Hernández-Gómez, S. and Gherardini, S. and Poggiali, F. and Cataliotti, F. S. and Trombettoni, A. and Cappellaro, P. and Fabbri, N.}, title = {Experimental test of exchange fluctuation relations in an open quantum system}, journal = {Phys. Rev. Research}, year = {2020}, volume = {2}, pages = {023327}, doi = {10.1103/PhysRevResearch.2.023327} } |
|
Phys. Rev. A 102, 010601 (2020) |
|
Abstract: Quantum simulation promises to address many challenges in fields ranging from quantum chemistry to material science and high-energy physics, and could be implemented in noisy intermediate-scale quantum devices. A challenge in building good digital quantum simulators is the fidelity of the engineered dynamics given a finite set of elementary operations. Here we present a framework for optimizing the order of operations based on a geometric picture, thus abstracting from the operation details and achieving computational efficiency. Based on this geometric framework, we provide two alternative second-order Trotter expansions: one with optimal fidelity at a short timescale, and the second robust at a long timescale. Thanks to the improved fidelity at different timescales, the two expansions we introduce can form the basis for experimental-constrained digital quantum simulation. | |
BibTeX:
@article{Liu20a, author = {Liu, Yi-Xiang and Hines, Jordan and Li, Zhi and Ajoy, Ashok and Cappellaro, Paola}, title = {High-fidelity Trotter formulas for digital quantum simulation}, journal = {Phys. Rev. A}, publisher = {American Physical Society}, year = {2020}, volume = {102}, pages = {010601}, doi = {10.1103/PhysRevA.102.010601} } |
|
Phys. Rev. X 10, 031003 (2020) |
|
Abstract: Quantum metrology makes use of coherent superpositions to detect weak signals. While in principle the sensitivity can be improved by increasing the density of sensing particles, in practice this improvement is severely hindered by interactions between them. Using a dense ensemble of interacting electronic spins in diamond, we demonstrate a novel approach to quantum metrology. It is based on a new method of robust quantum control, which allows us to simultaneously eliminate the undesired effects associated with spin-spin interactions, disorder and control imperfections, enabling a five-fold enhancement in coherence time compared to conventional control sequences. Combined with optimal initialization and readout protocols, this allows us to break the limit for AC magnetic field sensing imposed by interactions, opening a promising avenue for the development of solid-state ensemble magnetometers with unprecedented sensitivity. | |
BibTeX:
@article{Zhou20, author = {Zhou, Hengyun and Choi, Joonhee and Choi, Soonwon and Landig, Renate and Douglas, Alexander M. and Isoya, Junichi and Jelezko, Fedor and Onoda, Shinobu and Sumiya, Hitoshi and Cappellaro, Paola and Knowles, Helena S. and Park, Hongkun and Lukin, Mikhail D.}, title = {Quantum Metrology with Strongly Interacting Spin Systems}, journal = {Phys. Rev. X}, publisher = {American Physical Society}, year = {2020}, volume = {10}, pages = {031003}, doi = {10.1103/PhysRevX.10.031003} } |
|
In Proceedings of the International School of Physics "Enrico Fermi": Nanoscale Quantum Optics 204, 245 - 249 (2020) |
|
Abstract: Nitrogen-vacancy (NV) centers in diamond have emerged in the last decade as a prominent platform for quantum technologies. As for any qubit system, a good understanding of their local environment is crucial to build quantum devices protected from detrimental noise. Here, we describe in detail a method to spectroscopically characterize the spin bath around an NV center, even when the NV coherence time is short, and identify the coherent coupling with the nearest nuclear spins. In the regime of weak qubit-bath coupling, the acquired knowledge of the bath reliably predicts the qubit dynamics under different controls. | |
BibTeX:
@inproceedings{Hernandez20p, author = {S. Hernandez-Gomez, F. Poggiali, N. Fabbri, P. Cappellaro}, title = {Environment spectroscopy with an NV center in diamond}, booktitle = {Proceedings of the International School of Physics "Enrico Fermi": Nanoscale Quantum Optics}, year = {2020}, volume = {204}, pages = {245 - 249}, doi = {10.3254/ENFI200027}, url = {http://ebooks.iospress.nl/volumearticle/55677} } |
|
Phys. Rev. Lett. 124, 083602 (2020) |
|
Abstract: We experimentally demonstrate an approach to scale up quantum devices by harnessing spin defects in the environment of a quantum probe. We follow this approach to identify, locate, and control two electron-nuclear spin defects in the environment of a single nitrogen-vacancy center in diamond. By performing spectroscopy at various orientations of the magnetic field, we extract the unknown parameters of the hyperfine and dipolar interaction tensors, which we use to locate the two spin defects and design control sequences to initialize, manipulate, and readout their quantum state. Finally, we create quantum coherence among the three electron spins, paving the way for the creation of genuine tripartite entanglement. This approach will be useful in assembling multispin quantum registers for applications in quantum sensing and quantum information processing. | |
BibTeX:
@article{Cooper20, author = {Cooper, Alexandre and Sun, Won Kyu Calvin and Jaskula, Jean-Christophe and Cappellaro, Paola}, title = {Identification and Control of Electron-Nuclear Spin Defects in Diamond}, journal = {Phys. Rev. Lett.}, publisher = {American Physical Society}, year = {2020}, volume = {124}, pages = {083602}, doi = {10.1103/PhysRevLett.124.083602} } |
|
Phys. Rev. Lett. 124, 020504 (2020) |
|
Abstract: Quantum error correction is expected to be essential in large-scale quantum technologies. However, the substantial overhead of qubits it requires is thought to greatly limit its utility in smaller, near-term devices. Here we introduce a new family of special-purpose quantum error-correcting codes that offer an exponential reduction in overhead compared to the usual repetition code. They are tailored for a common and important source of decoherence in current experiments, whereby a register of qubits is subject to phase noise through coupling to a common fluctuator, such as a resonator or a spin defect. The smallest instance encodes one logical qubit into two physical qubits, and corrects decoherence to leading-order using a constant number of one- and two-qubit operations. More generally, while the repetition code on n qubits corrects errors to order t^O(n), with t the time between recoveries, our codes correct to order t^O(2^n). Moreover, they are robust to model imperfections in small- and intermediate-scale devices, where they already provide substantial gains in error suppression. As a result, these hardware-efficient codes open a potential avenue for useful quantum error correction in near-term, pre-fault tolerant devices. | |
BibTeX:
@article{Layden20, author = {Layden, David and Chen, Mo and Cappellaro, Paola}, title = {Efficient Quantum Error Correction of Dephasing Induced by a Common Fluctuator}, journal = {Phys. Rev. Lett.}, publisher = {American Physical Society}, year = {2020}, volume = {124}, pages = {020504}, doi = {10.1103/PhysRevLett.124.020504} } |
|
Phys. Rev. Lett. 124, 030601 (2020) |
|
Abstract: Evaluating the role of perturbations versus the intrinsic coherent dynamics in driving to equilibrium is of fundamental interest to understand quantum many-body thermalization, in the quest to build ever complex quantum devices. Here we introduce a protocol that scales down the coupling strength in a quantum simulator based on a solid-state nuclear spin system, leading to a longer decay time T2, while keeping perturbations associated to control error constant. We can monitor quantum information scrambling by measuring two powerful metrics, out-of-time-ordered correlators (OTOCs) and Loschmidt Echoes (LEs). While OTOCs reveal quantum information scrambling involving hundreds of spins, the LE decay quantifies, via the time scale T3, how well the scrambled information can be recovered through time reversal. We find that when the interactions dominate the perturbation, the LE decay rate only depends on the interactions themselves, T3 ~ T2, and not on the perturbation. Then, in an unbounded many-spin system, decoherence can achieve a perturbation-independent regime, with a rate only related to the local second moment of the Hamiltonian. | |
BibTeX:
@article{Sanchez20, author = {Sánchez, C. M. and Chattah, A. K. and Wei, K. X. and Buljubasich, L. and Cappellaro, P. and Pastawski, H. M.}, title = {Perturbation Independent Decay of the Loschmidt Echo in a Many-Body System}, journal = {Phys. Rev. Lett.}, publisher = {American Physical Society}, year = {2020}, volume = {124}, pages = {030601}, doi = {10.1103/PhysRevLett.124.030601} } |
|
Phys. Rev. A 101, 012319 (2020) |
|
Abstract: Entanglement, while being critical in many quantum applications, is difficult to characterize experimentally. While entanglement witnesses based on the fidelity to the target entangled state are efficient detectors of entanglement, they in general underestimate the amount of entanglement due to errors during state preparation and measurement. Here, to improve entanglement detection, we introduce a 'subspace' witness that can detect a broader class of entangled states than the conventional state-fidelity witnesses, while still remaining more efficient than state tomography. We experimentally demonstrate the advantages of the subspace witness by generating and detecting entanglement with a hybrid, two-qubit system composed of electronic spins in diamond. We further extend the notion of subspace witness to specific genuine multipartite entangled (GME) states such as GHZ, W, and Dicke states, and motivate the choice of the metric based on quantum information tasks such as entanglement-enhanced sensing. We expect the straightforward and efficient implementation of subspace witnesses would be beneficial in detecting specific GME states in noisy, intermediate-scale quantum processors with a hundred qubits. | |
BibTeX:
@article{Sun20, author = {Sun, Won Kyu Calvin and Cooper, Alexandre and Cappellaro, Paola}, title = {Improved entanglement detection with subspace witnesses}, journal = {Phys. Rev. A}, publisher = {American Physical Society}, year = {2020}, volume = {101}, pages = {012319}, doi = {10.1103/PhysRevA.101.012319} } |
|
Quantum Science and Technology 5, 025004 (2020) |
|
Abstract: Quantum error correction (QEC) codes are usually designed to correct errors regardless of their physical origins. In large-scale devices, this is an essential feature. In smaller-scale devices, however, the main error sources are often understood, and this knowledge could be exploited for more efficient error correction. Optimizing the QEC protocol is therefore a promising strategy in smaller devices. Typically, this involves tailoring the protocol to a given decoherence channel by solving an appropriate optimization problem. Here we introduce a new optimization-based approach, which maximizes the robustness to faults in the recovery. Our approach is inspired by recent experiments, where such faults have been a significant source of logical errors. We illustrate this approach with a three-qubit model, and show how near-term experiments could benefit from more robust QEC protocols. | |
BibTeX:
@article{Layden20q, author = {David Layden and Louisa Ruixue Huang and Paola Cappellaro}, title = {Robustness-optimized quantum error correction}, journal = {Quantum Science and Technology}, publisher = {IOP Publishing}, year = {2020}, volume = {5}, number = {2}, pages = {025004}, doi = {10.1088/2058-9565/ab79b2} } |
|
Machine Learning: Science and Technology 1, 015003 (2020) |
|
Abstract: Single-shot readout is a key component for scalable quantum information processing. However, many solid-state qubits with favorable properties lack the single-shot readout capability. One solution is to use the repetitive quantum-non-demolition readout technique, where the qubit is correlated with an ancilla, which is subsequently read out. The readout fidelity is therefore limited by the back-action on the qubit from the measurement. Traditionally, a threshold method is taken, where only the total photon count is used to discriminate qubit state, discarding all the information of the back-action hidden in the time trace of repetitive readout measurement. Here we show by using machine learning (ML), one obtains higher readout fidelity by taking advantage of the time trace data. ML is able to identify when back-action happened, and correctly read out the original state. Since the information is already recorded (but usually discarded), this improvement in fidelity does not consume additional experimental time, and could be directly applied to preparation-by-measurement and quantum metrology applications involving repetitive readout. | |
BibTeX:
@article{Liu20, author = {Genyue Liu and Mo Chen and Yi-Xiang Liu and David Layden and Paola Cappellaro}, title = {Repetitive readout enhanced by machine learning}, journal = {Machine Learning: Science and Technology}, publisher = {IOP Publishing}, year = {2020}, volume = {1}, number = {1}, pages = {015003}, doi = {10.1088/2632-2153/ab4e24} } |
|
IEEE Transactions on Automatic Control In IEEE Transactions on Automatic Control , 1 (2020) |
|
Abstract: The identifiability of a system is concerned with whether the unknown parameters in the system can be uniquely determined with all the possible data generated by a certain experimental setting. In this paper, we generalize the identifiability test based on the Similarity Transformation Approach (STA) in classical control theory and extend it to the domain of quantum Hamiltonian identification. We employ STA to prove the identifiability of spin-1/2 chain systems with arbitrary dimension assisted by single-qubit probes. We further extend the traditional STA method by proposing a Structure Preserving Transformation (SPT) method for non-minimal systems. We use the SPT method to introduce an indicator for the existence of economic quantum Hamiltonian identification algorithms, whose computational complexity directly depends on the number of unknown parameters (which could be much smaller than the system dimension). Finally, we give an example of such an economic Hamiltonian identification algorithm and perform simulations to demonstrate its effectiveness. | |
BibTeX:
@article{Wang20, author = {Wang, Y. and Dong, D. and Sone, A. and Petersen, I. R. and Yonezawa, H. and Cappellaro, P.}, title = {Quantum Hamiltonian Identifiability via a Similarity Transformation Approach and Beyond}, booktitle = {IEEE Transactions on Automatic Control}, journal = {IEEE Transactions on Automatic Control}, year = {2020}, pages = {1}, doi = {10.1109/TAC.2020.2973582} } |
|
2019 | UP ↑ |
Phys. Rev. B 100, 214203 (2019) |
|
Abstract: Many-body localization (MBL), characterized by the absence of thermalization and the violation of conventional thermodynamics, has elicited much interest both as a fundamental physical phenomenon and for practical applications in quantum information. A phenomenological model, which describes the system using a complete set of local integrals of motion (LIOMs), provides a powerful tool to understand MBL, but can be usually only computed approximately. Here we explicitly compute a complete set of LIOMs with a non-perturbative approach, by maximizing the overlap between LIOMs and physical spin operators in real space. The set of LIOMs satisfies the desired exponential decay of weight of LIOMs in real-space. This LIOM construction enables a direct mapping from the real space Hamiltonian to the phenomenological model and thus enables studying the localized Hamiltonian and the system dynamics. We can thus study and compare the localization lengths extracted from the LIOM weights, their interactions, and dephasing dynamics, revealing interesting aspects of many-body localization. Our scheme is immune to accidental resonances and can be applied even at phase transition point, providing a novel tool to study the microscopic features of the phenomenological model of MBL. | |
BibTeX:
@article{Peng19, author = {Pai Peng and Zeyang Li and Haoxiong Yan and Ken Xuan Wei and Paola Cappellaro}, title = {Comparing many-body localization lengths via non-perturbative construction of local integrals of motion}, journal = {Phys. Rev. B}, year = {2019}, volume = {100}, pages = {214203}, doi = {10.1103/PhysRevB.100.214203} } |
|
J. Phys. Comms. 3, 095016- (2019) |
|
Abstract: Solid-state spins such as nitrogen-vacancy (NV) center are promising platforms for large-scale quantum networks. Despite the optical interface of NV center system, however, the significant attenuation of its zero-phonon-line photon in optical fiber prevents the network extended to long distances. Therefore a telecom-wavelength photon interface would be essential to reduce the photon loss in transporting quantum information. Here we propose an efficient scheme for coupling telecom photon to NV center ensembles mediated by rare-earth doped crystal. Specifically, we proposed protocols for high fidelity quantum state transfer and entanglement generation with parameters within reach of current technologies. Such an interface would bring new insights into future implementations of long-range quantum network with NV centers in diamond acting as quantum nodes. | |
BibTeX:
@article{Li19, author = {Li, Changhao and Cappellaro, Paola}, title = {Telecom photon interface of solid-state quantum nodes}, journal = {J. Phys. Comms.}, publisher = {IOP Publishing}, year = {2019}, volume = {3}, number = {9}, pages = {095016--} } |
|
Nano Lett. 19, 7342-7348 (2019) |
|
Abstract: Sensing the local environment through the motional response of small molecules lays the foundation of many fundamental technologies. The information on local viscosity, for example, is contained in the random rotational Brownian motions of molecules. However, detection of the motions is challenging for molecules with sub-nanometer scale or high motional rates. Here we propose and experimentally demonstrate a novel method of detecting fast rotational Brownian motions of small magnetic molecules. With electronic spins as sensors, we are able to detect changes in motional rates, which yield different noise spectra and therefore different relaxation signals of the sensors. As a proof-of-principle demonstration, we experimentally implemented this method to detect the motions of gadolinium (Gd) complex molecules with nitrogen-vacancy (NV) centers in nanodiamonds. With all-optical measurements of the NV centers’ longitudinal relaxation, we distinguished binary solutions with varying viscosities. Our method paves a new way for detecting fast motions of sub-nanometer sized magnetic molecules with better spatial resolution than conventional optical methods. It also provides a new tool in designing better contrast agents in magnetic resonance imaging. Sensing the local environment through the motional response of small molecules lays the foundation of many fundamental technologies. The information on local viscosity, for example, is contained in the random rotational Brownian motions of molecules. However, detection of the motions is challenging for molecules with sub-nanometer scale or high motional rates. Here we propose and experimentally demonstrate a novel method of detecting fast rotational Brownian motions of small magnetic molecules. With electronic spins as sensors, we are able to detect changes in motional rates, which yield different noise spectra and therefore different relaxation signals of the sensors. As a proof-of-principle demonstration, we experimentally implemented this method to detect the motions of gadolinium (Gd) complex molecules with nitrogen-vacancy (NV) centers in nanodiamonds. With all-optical measurements of the NV centers’ longitudinal relaxation, we distinguished binary solutions with varying viscosities. Our method paves a new way for detecting fast motions of sub-nanometer sized magnetic molecules with better spatial resolution than conventional optical methods. It also provides a new tool in designing better contrast agents in magnetic resonance imaging. |
|
BibTeX:
@article{Li19b, author = {Li, Changhao and Chen, Mo and Lyzwa, Dominika and Cappellaro, Paola}, title = {All-Optical Quantum Sensing of Rotational Brownian Motion of Magnetic Molecules}, journal = {Nano Lett.}, year = {2019}, volume = {19}, number = {10}, pages = {7342--7348}, doi = {10.1021/acs.nanolett.9b02960} } |
|
Phys. Rev. Applied 12, 044047 (2019) |
|
Abstract: The performance of solid-state quantum sensors based on electronic spin defects is often limited by the presence of environmental spin impurities that cause decoherence. A promising approach to improve these quantum sensors is to convert environment spins into useful resources for sensing, in particular, entangled states. However, the sensitivity enhancement that can be achieved from entangled states is limited by experimental constraints, such as control errors, decoherence, and time overheads. Here we experimentally demonstrate the efficient use of an unknown electronic spin defect in the proximity of a nitrogen-vacancy center in diamond to achieve both an entangled quantum sensor and a quantum memory for readout. We show that, whereas entanglement alone does not provide an enhancement in sensitivity, combining both entanglement and repetitive readout achieves an enhancement in performance over the use of a single-spin sensor, and more broadly we discuss regimes where sensitivity could be enhanced. Our results critically highlight the challenges in improving quantum sensors using entangled states of electronic spins, while providing an important benchmark in the quest for entanglement-assisted metrology. | |
BibTeX:
@article{Cooper19, author = {Cooper, Alexandre and Sun, Won Kyu Calvin and Jaskula, Jean-Christophe and Cappellaro, Paola}, title = {Environment-assisted Quantum-enhanced Sensing with Electronic Spins in Diamond}, journal = {Phys. Rev. Applied}, publisher = {American Physical Society}, year = {2019}, volume = {12}, pages = {044047}, doi = {10.1103/PhysRevApplied.12.044047} } |
|
Phys. Rev. App. 11, 054010 (2019) |
|
Abstract: Quantum sensors, such as the Nitrogen Vacancy (NV) color center in diamond, are known for their exquisite sensitivity, but their performance is degraded by noise. To improve the long-term robustness of a quantum sensor, here we realize an integrated combinatorial spin sensor in the same micrometer-scale footprint, which exploits two different spin sensitivity to distinct physical quantities to stabilize one spin sensor with local information collected in realtime via the second sensor. We show that we can use the electronic spins of a large ensemble of NV centers as sensor of the local magnetic field fluctuations, affecting both spin sensors, in order to stabilize the output signal of interleaved Ramsey sequences performed on the 14N nuclear spin. An envisioned application of such a device is to sense rotation rates with a stability of several days, allowing navigation with limited or no requirement of geo-localization. Our results would enable stable rotation sensing for over several hours, which already reflects better performance than MEMS gyroscopes of comparable sensitivity and size. | |
BibTeX:
@article{Jaskula19, author = {Jean-Christophe Jaskula and Kasturi Saha and Ashok Ajoy and Daniel J. Twitchen and Matthew Markham and Paola Cappellaro}, title = {Cross-sensor feedback stabilization of an emulated quantum spin gyroscope}, journal = {Phys. Rev. App.}, publisher = {American Physical Society}, year = {2019}, volume = {11}, pages = {054010}, doi = {10.1103/PhysRevApplied.11.054010} } |
|
In Proceedings of SPIE Optical, Opto-Atomic, and Entanglement-Enhanced Precision Metrology, Volume 10934, 1J (2019) |
|
Abstract: Quantum metrology has many important applications in science and technology, ranging from frequency spectroscopy to gravitational wave detection. Quantum mechanics imposes a fundamental limit on measurement precision, called the Heisenberg limit, which can be achieved for noiseless quantum systems, but is not achievable in general for systems subject to noise. Here we study how measurement precision can be enhanced through quantum error correction, a general method for protecting a quantum system from the damaging effects of noise. We find a necessary and sufficient condition for achieving the Heisenberg limit using quantum probes subject to Markovian noise, assuming that noiseless ancilla systems are available, and that fast, accurate quantum processing can be performed. When the sufficient condition is satisfied, the quantum error-correcting code achieving the best possible precision can be found by solving a semidefinite program. We also show that noiseless ancilla are not needed when the signal Hamiltonian and the error operators commute. Finally we provide two explicit, archetypal examples of quantum sensors: qubits undergoing dephasing and a lossy bosonic mode. | |
BibTeX:
@inproceedings{Zhou19, author = {Sisi Zhou, David Layden, Mengzhen Zhang, John Preskill, Paola Cappellaro, Liang Jiang}, title = {Error-corrected quantum sensing}, booktitle = {SPIE Optical, Opto-Atomic, and Entanglement-Enhanced Precision Metrology}, publisher = {SPIE}, year = {2019}, volume = {10934}, pages = {109341J}, doi = {10.1117/12.2511587} } |
|
Phys. Rev. A 99, 052318 (2019) |
|
Abstract: Nonclassical correlation beyond entanglement might provide a resource in quantum information tasks, such as quantum computation or quantum metrology. Quantum discord is a measure of nonclassical correlations beyond entanglement. Exploring the operational meaning of quantum discord as a resource in quantum information processing tasks, such as quantum metrology, is of essential importance to our understanding of nonclassical correlation. In our recent work [Phys. Rev. A, 98, 012115 (2018)], we have demonstrated that the diagonal discord plays a role in enhancing the high-temperature sensitivity of the greedy local thermometry scheme, where one measures the subsystems sequentially with the local optimal measurement. In this paper, we extend our results to a general greedy local parameter estimation scenario. In particular, we introduce a quantum discord, which we call discord for local metrology, to quantify the nonclassical correlations induced by the local optimal measurement on the subsystem. We demonstrate explicitly that discord for local metrology plays a role in sensitivity enhancement in the high-temperature limit by showing its relation to loss in quantum Fisher information. In particular, it coincides with diagonal discord for estimating a linear coupling parameter. | |
BibTeX:
@article{Sone19, author = {Sone, Akira and Zhuang, Quntao and Li, Changhao and Liu, Yi-Xiang and Cappellaro, Paola}, title = {Nonclassical correlations for quantum metrology in thermal equilibrium}, journal = {Phys. Rev. A}, year = {2019}, volume = {99}, pages = {052318}, doi = {10.1103/PhysRevA.99.052318} } |
|
Quantum Information and Measurement (QIM) V: Quantum Technologies In Quantum Information and Measurement (QIM) V: Quantum Technologies , S3C.2 (2019) |
|
Abstract: We devise a robust quantum sensing scheme based on optimal control. We experimentally demonstrate sensitivity enhancement of diamond spin-qubits sensors to measure ultraweak time-varying magnetic fields in noisy environments. | |
BibTeX:
@inproceedings{Poggiali19, author = {Francesco Poggiali and Santiago Hern\'{a}ndez-G\'{o}mez and Paola Cappellaro and Nicole Fabbri}, title = {Optimal control of diamond spin qubits for quantum sensing in noisy environments}, booktitle = {Quantum Information and Measurement (QIM) V: Quantum Technologies}, journal = {Quantum Information and Measurement (QIM) V: Quantum Technologies}, publisher = {Optical Society of America}, year = {2019}, pages = {S3C.2}, doi = {10.1364/QIM.2019.S3C.2} } |
|
Phys. Rev. Lett. 122, 100501 (2019) |
|
Abstract: Sensing static magnetic fields with high sensitivity and spatial resolution is critical to many applications in fundamental physics, bioimaging, and materials science. Even more beneficial would be full vector magnetometry with nanoscale spatial resolution. Several versatile magnetometry platforms have emerged over the past decade, such as electronic spins associated with nitrogen vacancy (NV) centers in diamond. Achieving vector magnetometry has, however, often required using an ensemble of sensors or degrading the sensitivity. Here we introduce a hybrid magnetometry platform, consisting of a sensor and an ancillary qubit, that allows vector magnetometry of static fields. While more generally applicable, we demonstrate the method for an electronic NV sensor and a nuclear spin qubit. In particular, sensing transverse fields relies on frequency up-conversion of the dc fields through the ancillary qubit, allowing quantum lock-in detection with low-frequency noise rejection. In combination with the Ramsey detection of longitudinal fields, our frequency up-conversion scheme delivers a sensitive technique for vector dc magnetometry at the nanoscale. | |
BibTeX:
@article{Liu19, author = {Liu, Yi-Xiang and Ajoy, Ashok and Cappellaro, Paola}, title = {Nanoscale Vector dc Magnetometry via Ancilla-Assisted Frequency Up-Conversion}, journal = {Phys. Rev. Lett.}, publisher = {American Physical Society}, year = {2019}, volume = {122}, pages = {100501}, doi = {10.1103/PhysRevLett.122.100501} } |
|
Phys. Rev. Lett. 122, 013205 (2019) |
|
Abstract: We present a protocol to selectively decouple, recouple, and engineer effective interactions in mesoscopic dipolar spin networks. In particular, we develop a versatile protocol that relies upon magic angle spinning to perform Hamiltonian engineering. By using global control fields in conjunction with a local actuator, such as a diamond nitrogen vacancy center located in the vicinity of a nuclear spin network, both global and local control over the effective couplings can be achieved. We show that the resulting effective Hamiltonian can be well understood within a simple, intuitive geometric picture, and corroborate its validity by performing exact numerical simulations in few-body systems. Applications of our method are in the emerging fields of two-dimensional room temperature quantum simulators in diamond platforms, as well as in molecular magnet systems. | |
BibTeX:
@article{Ajoy19, author = {Ajoy, A. and Bissbort, U. and Poletti, D. and Cappellaro, P.}, title = {Selective Decoupling and Hamiltonian Engineering in Dipolar Spin Networks}, journal = {Phys. Rev. Lett.}, publisher = {American Physical Society}, year = {2019}, volume = {122}, pages = {013205}, doi = {10.1103/PhysRevLett.122.013205} } |
|
Phys. Rev. Lett. 122, 040502 (2019) |
|
Abstract: Quantum error correction has recently emerged as a tool to enhance quantum sensing under Markovian noise. It works by correcting errors in a sensor while letting a signal imprint on the logical state. This approach typically requires a specialized error-correcting code, as most existing codes correct away both the dominant errors and the signal. To date, however, few such specialized codes are known, among which most require noiseless, controllable ancillas. We show here that such ancillas are not needed when the signal Hamiltonian and the error operators commute, a common limiting type of decoherence in quantum sensors. We give a semidefinite program for finding optimal ancilla-free sensing codes in general, as well as closed-form codes for two common sensing scenarios: qubits undergoing dephasing, and a lossy bosonic mode. Finally, we analyze the sensitivity enhancement offered by the qubit code under arbitrary spatial noise correlations, beyond the ideal limit of orthogonal signal and noise operators. | |
BibTeX:
@article{Layden19, author = {Layden, David and Zhou, Sisi and Cappellaro, Paola and Jiang, Liang}, title = {Ancilla-Free Quantum Error Correction Codes for Quantum Metrology}, journal = {Phys. Rev. Lett.}, publisher = {American Physical Society}, year = {2019}, volume = {122}, pages = {040502}, doi = {10.1103/PhysRevLett.122.040502} } |
|
Phys. Rev. Lett. 123, 090605 (2019) |
|
Abstract: How a many-body quantum system thermalizes—or fails to do so—under its own interaction is a fundamental yet elusive concept. Here we demonstrate nuclear magnetic resonance observation of the emergence of prethermalization by measuring out-of-time ordered correlations. We exploit Hamiltonian engineering techniques to tune the strength of spin-spin interactions and of a transverse magnetic field in a spin chain system, as well as to invert the Hamiltonian sign to reveal out-of-time ordered correlations. At large fields, we observe an emergent conserved quantity due to prethermalization, which can be revealed by an early saturation of correlations. Our experiment not only demonstrates a new protocol to measure out-of-time ordered correlations, but also provides new insights in the study of quantum thermodynamics. | |
BibTeX:
@article{Wei19, author = {Wei, K.~X. and Peng, P. and Shtanko, O. and Marvian, I. and Lloyd, S. and Ramanathan, C. and Cappellaro, P.}, title = { Emergent Prethermalization Signatures in Out-of-Time Ordered Correlations }, journal = {Phys. Rev. Lett.}, publisher = {American Physical Society}, year = {2019}, volume = {123}, pages = {090605}, doi = {10.1103/PhysRevLett.123.090605} } |
|
2018 | UP ↑ |
New J. Phys. 20, 063011 (2018) |
|
Abstract: Quantum memories are critical for solid-state quantum computing devices and a good quantum memory requires both long storage time and fast read/write operations. A promising system is the nitrogen-vacancy (NV) center in diamond, where the NV electronic spin serves as the computing qubit and a nearby nuclear spin as the memory qubit. Previous works used remote, weakly coupled 13C nuclear spins, trading read/write speed for long storage time. Here we focus instead on the intrinsic strongly coupled 14N nuclear spin. We first quantitatively understand its decoherence mechanism, identifying as its source the electronic spin that acts as a quantum fluctuator. We then propose a scheme to protect the quantum memory from the fluctuating noise by applying dynamical decoupling on the environment itself. We demonstrate a factor of 3 enhancement of the storage time in a proof-of-principle experiment, showing the potential for a quantum memory that combines fast operation with long coherence time. | |
BibTeX:
@article{Chen18, author = {Chen, M. and Sun, W.~K.~C. and Saha, K. and Jaskula, J.-C. and Cappellaro, P.}, title = {Protecting solid-state spins from a strongly coupled environment}, journal = {New J. Phys.}, year = {2018}, volume = {20}, number = {6}, pages = {063011}, doi = {10.1088/1367-2630/aac542} } |
|
Phys. Rev. B 98, 214307 (2018) |
|
Abstract: Knowing a quantum system's environment is critical for its practical use as a quantum device. Qubit sensors can reconstruct the noise spectral density of a classical bath, provided long enough coherence time. Here, we present a protocol that can unravel the characteristics of a more complex environment, comprising both unknown coherently coupled quantum systems, and a larger quantum bath that can be modeled as a classical stochastic field. We exploit the rich environment of a nitrogen-vacancy center in diamond, tuning the environment behavior with a bias magnetic field, to experimentally demonstrate our method. We show how to reconstruct the noise spectral density even when limited by relatively short coherence times, and identify the local spin environment. Importantly, we demonstrate that the reconstructed model can have predictive power, describing the spin qubit dynamics under control sequences not used for noise spectroscopy, a feature critical for building robust quantum devices. At lower bias fields, where the effects of the quantum nature of the bath are more pronounced, we find that more than a single classical noise model are needed to properly describe the spin coherence under different controls, due to the back action of the qubit onto the bath. | |
BibTeX:
@article{Hernandez18, author = {Hernández-Gómez, S. and Poggiali, F. and Cappellaro, P. and Fabbri, N.}, title = {Noise spectroscopy of a quantum-classical environment with a diamond qubit}, journal = {Phys. Rev. B}, publisher = {American Physical Society}, year = {2018}, volume = {98}, pages = {214307}, doi = {10.1103/PhysRevB.98.214307} } |
|
Quantum Inf. Process. 17, 88 (2018) |
|
Abstract: Time-optimal control theory provides recipes to achieve quantum operations with high fidelity and speed, as required in quantum technologies such as quantum sensing and computation. While technical advances have achieved the ultrastrong driving regime in many physical systems, these capabilities have yet to be fully exploited for the precise control of quantum systems, as other limitations, such as the generation of higher harmonics or the finite response time of the control apparatus, prevent the implementation of theoretical time-optimal control. Here we present a method to achieve time-optimal control of qubit systems that can take advantage of fast driving beyond the rotating wave approximation. We exploit results from time-optimal control theory to design driving protocols that can be implemented with realistic, finite-bandwidth control fields, and we find a relationship between bandwidth limitations and achievable control fidelity. | |
BibTeX:
@article{Hirose18, author = {Hirose, M. and Cappellaro, P.}, title = {Time-optimal control with finite bandwidth}, journal = {Quantum Inf. Process.}, year = {2018}, volume = {17}, pages = {88}, doi = {10.1007/s11128-018-1845-6} } |
|
npj Quantum Information 4, 30 (2018) |
|
Abstract: Quantum systems can be used to measure various quantities in their environment with high precision. Often, however, their sensitivity is limited by the decohering effects of this same environment. Dynamical decoupling schemes are widely used to filter environmental noise from signals, but their performance is limited by the spectral properties of the signal and noise at hand. Quantum error correction schemes have therefore emerged as a complementary technique without the same limitations. To date, however, they have failed to correct the dominant noise type in many quantum sensors, which couples to each qubit in a sensor in the same way as the signal. Here we show how quantum error correction can correct for such noise, which dynamical decoupling can only partially address. Whereas dynamical decoupling exploits temporal noise correlations in signal and noise, our scheme exploits spatial correlations. We give explicit examples in small quantum devices and demonstrate a method by which error-correcting codes can be tailored to their noise. | |
BibTeX:
@article{Layden18, author = {Layden, David and Cappellaro, Paola}, title = {Spatial noise filtering through error correction for quantum sensing}, journal = {npj Quantum Information}, year = {2018}, volume = {4}, number = {1}, pages = {30}, doi = {10.1038/s41534-018-0082-2} } |
|
Opt. Express 26, 80-89 (2018) |
|
Abstract: The practical implementation of many quantum technologies relies on the development of robust and bright single photon sources that operate at room temperature. The negatively charged silicon-vacancy (SiV-) color center in diamond is a possible candidate for such a single photon source. However, due to the high refraction index mismatch to air, color centers in diamond typically exhibit low photon out-coupling. An additional shortcoming is due to the random localization of native defects in the diamond sample. Here we demonstrate deterministic implantation of Si ions with high conversion efficiency to single SiV− centers, targeted to fabricated nanowires. The co-localization of single SiV- centers with the nanostructures yields a ten times higher light coupling efficiency than for single SiV- centers in bulk diamond. This enhanced photon out-coupling, together with the intrinsic scalability of the SiV− creation method, enables a new class of devices for integrated photonics and quantum science. | |
BibTeX:
@article{Marseglia18, author = {Marseglia, L. and Saha, K. and Ajoy, A. and Schroeder, T. and Englund, D. and Jelezko, F. and Walsworth, R. and Pacheco, J. L. and Perry, D. L. and Bielejec, E. S. and Cappellaro, P.}, title = {Bright nanowire single photon source based on SiV centers in diamond}, journal = {Opt. Express}, publisher = {OSA}, year = {2018}, volume = {26}, number = {1}, pages = {80--89} } |
|
Phys. Rev. X 8, 021059 (2018) |
|
Abstract: Quantum systems can be exquisite sensors thanks to their sensitivity to external perturbations. This same characteristic also makes them fragile to external noise. Quantum control can tackle the challenge of protecting a quantum sensor from environmental noise, while strongly coupling the sensor with the field to be measured. As the compromise between these two conflicting requirements does not always have an intuitive solution, optimal control based on a numerical search could prove very effective. Here, we adapt optimal control theory to the quantum-sensing scenario by introducing a cost function that, unlike the usual fidelity of operation, correctly takes into account both the field to be measured and the environmental noise. We experimentally implement this novel control paradigm using a nitrogen vacancy center in diamond, finding improved sensitivity to a broad set of time-varying fields. The demonstrated robustness and efficiency of the numerical optimization, as well as the sensitivity advantage it bestows, will prove beneficial to many quantum-sensing applications. | |
BibTeX:
@article{Poggiali18, author = {Poggiali, F. and Cappellaro, P. and Fabbri, N.}, title = {Optimal Control for One-Qubit Quantum Sensing}, journal = {Phys. Rev. X}, publisher = {American Physical Society}, year = {2018}, volume = {8}, pages = {021059}, doi = {10.1103/PhysRevX.8.021059} } |
|
Phys. Rev. A 98, 012115 (2018) |
|
Abstract: When quantum information is spread over a system through nonclassical correlation, it makes retrieving information by local measurements difficult—making global measurement necessary for optimal parameter estimation. In this paper, we consider temperature estimation of a system in a Gibbs state and quantify the separation between the estimation performance of the global optimal measurement scheme and a greedy local measurement scheme by diagonal quantum discord. In a greedy local scheme, instead of global measurements, one performs sequential local measurement on subsystems, which is potentially enhanced by feed-forward communication. We show that, for finite-dimensional systems, diagonal discord quantifies the difference in the quantum Fisher information quantifying the precision limits for temperature estimation of these two schemes, and we analytically obtain the relation in the high-temperature limit. We further verify this result by employing the examples of spins with Heisenberg's interaction. | |
BibTeX:
@article{Sone18b, author = {Sone, Akira and Zhuang, Quntao and Cappellaro, Paola}, title = {Quantifying precision loss in local quantum thermometry via diagonal discord}, journal = {Phys. Rev. A}, publisher = {American Physical Society}, year = {2018}, volume = {98}, pages = {012115}, doi = {10.1103/PhysRevA.98.012115} } |
|
Phys. Rev. Lett. 120, 070501 (2018) |
|
Abstract: Characterizing out-of-equilibrium many-body dynamics is a complex but crucial task for quantum applications and understanding fundamental phenomena. A central question is the role of localization in quenching thermalization in many-body systems and whether such localization survives in the presence of interactions. Probing this question in real systems necessitates the development of an experimentally measurable metric that can distinguish between different types of localization. While it is known that the localized phase of interacting systems [many-body localization (MBL)] exhibits a long-time logarithmic growth in entanglement entropy that distinguishes it from the noninteracting case of Anderson localization (AL), entanglement entropy is difficult to measure experimentally. Here, we present a novel correlation metric, capable of distinguishing MBL from AL in high-temperature spin systems. We demonstrate the use of this metric to detect localization in a natural solid-state spin system using nuclear magnetic resonance (NMR). We engineer the natural Hamiltonian to controllably introduce disorder and interactions, and observe the emergence of localization. In particular, while our correlation metric saturates for AL, it slowly keeps increasing for MBL, demonstrating analogous features to entanglement entropy, as we show in simulations. Our results show that our NMR techniques, akin to measuring out-of-time correlations, are well suited for studying localization in spin systems. | |
BibTeX:
@article{Wei18, author = {Wei, Ken Xuan and Ramanathan, Chandrasekhar and Cappellaro, Paola}, title = {Exploring Localization in Nuclear Spin Chains}, journal = {Phys. Rev. Lett.}, publisher = {American Physical Society}, year = {2018}, volume = {120}, pages = {070501}, doi = {10.1103/PhysRevLett.120.070501} } |
|
2017 | UP ↑ |
Proc. Nat. Acad. Sc. 114, 2149–2153 (2017) |
|
Abstract: Recent advances in engineering and control of nanoscale quantum sensors have opened new paradigms in precision metrology. Unfortunately, hardware restrictions often limit the sensor performance. In nanoscale magnetic resonance probes, for instance, finite sampling times greatly limit the achievable sensitivity and spectral resolution. Here we introduce a technique for coherent quantum interpolation that can overcome these problems. Using a quantum sensor associated with the nitrogen vacancy center in diamond, we experimentally demonstrate that quantum interpolation can achieve spectroscopy of classical magnetic fields and individual quantum spins with orders of magnitude finer frequency resolution than conventionally possible. Not only is quantum interpolation an enabling technique to extract structural and chemical information from single biomolecules, but it can be directly applied to other quantum systems for superresolution quantum spectroscopy. | |
BibTeX:
@article{Ajoy17, author = {Ajoy, Ashok and Liu, Yi-Xiang and Saha, Kasturi and Marseglia, Luca and Jaskula, Jean-Christophe and Bissbort, Ulf and Cappellaro, Paola}, title = {Quantum interpolation for high-resolution sensing}, journal = {Proc. Nat. Acad. Sc.}, year = {2017}, volume = {114}, number = {9}, pages = {2149–2153}, doi = {10.1073/pnas.1610835114} } |
|
Thesis at: Massachusetts Institute of Technology, (2017) |
|
BibTeX:
@mastersthesis{Alsid17t, author = {Alsid, Scott T}, title = {Optimizing chemical-vapor-deposition diamond for nitrogen-vacancy center ensemble magnetometry}, school = {Massachusetts Institute of Technology}, year = {2017} } |
|
Phys. Rev. A 95, 022335 (2017) |
|
Abstract: We study the Hamiltonian identifiability of a many-body spin-1/2 system assisted by the measurement on a single quantum probe based on the eigensystem realization algorithm approach employed in Zhang and Sarovar, Phys. Rev. Lett. 113, 080401 (2014). We demonstrate a potential application of Gröbner basis to the identifiability test of the Hamiltonian, and provide the necessary experimental resources, such as the lower bound in the number of the required sampling points, the upper bound in total required evolution time, and thus the total measurement time. Focusing on the examples of the identifiability in the spin-chain model with nearest-neighbor interaction, we classify the spin-chain Hamiltonian based on its identifiability, and provide the control protocols to engineer the nonidentifiable Hamiltonian to be an identifiable Hamiltonian. | |
BibTeX:
@article{Sone17, author = {Sone, Akira and Cappellaro, Paola}, title = {Hamiltonian identifiability assisted by a single-probe measurement}, journal = {Phys. Rev. A}, year = {2017}, volume = {95}, pages = {022335}, doi = {10.1103/PhysRevA.95.022335} } |
|
Phys. Rev. A 96, 062334 (2017) |
|
Abstract: Estimating the dimension of an Hilbert space is an important component of quantum system identification. In quantum technologies, the dimension of a quantum system (or its corresponding accessible Hilbert space) is an important resource, as larger dimensions determine, e.g., the performance of quantum computation protocols or the sensitivity of quantum sensors. Despite being a critical task in quantum system identification, estimating the Hilbert space dimension is experimentally challenging. While there have been proposals for various dimension witnesses capable of putting a lower bound on the dimension from measuring collective observables that encode correlations, in many practical scenarios, especially for multiqubit systems, the experimental control might not be able to engineer the required initialization, dynamics, and observables. Here we propose a more practical strategy that relies not on directly measuring an unknown multiqubit target system, but on the indirect interaction with a local quantum probe under the experimenter's control. Assuming only that the interaction model is given and the evolution correlates all the qubits with the probe, we combine a graph-theoretical approach and realization theory to demonstrate that the system dimension can be exactly estimated from the model order of the system. We further analyze the robustness in the presence of background noise of the proposed estimation method based on realization theory, finding that despite stringent constrains on the allowed noise level, exact dimension estimation can still be achieved. | |
BibTeX:
@article{Sone17a, author = {Sone, Akira and Cappellaro, Paola}, title = {Exact dimension estimation of interacting qubit systems assisted by a single quantum probe}, journal = {Phys. Rev. A}, publisher = {American Physical Society}, year = {2017}, volume = {96}, pages = {062334}, doi = {10.1103/PhysRevA.96.062334} } |
|
Rev. Mod. Phys. 89, 035002 (2017) |
|
Abstract: “Quantum sensing” describes the use of a quantum system, quantum properties, or quantum phenomena to perform a measurement of a physical quantity. Historical examples of quantum sensors include magnetometers based on superconducting quantum interference devices and atomic vapors or atomic clocks. More recently, quantum sensing has become a distinct and rapidly growing branch of research within the area of quantum science and technology, with the most common platforms being spin qubits, trapped ions, and flux qubits. The field is expected to provide new opportunities—especially with regard to high sensitivity and precision—in applied physics and other areas of science. This review provides an introduction to the basic principles, methods, and concepts of quantum sensing from the viewpoint of the interested experimentalist. | |
BibTeX:
@article{Degen17, author = {Degen, C. L. and Reinhard, F. and Cappellaro, P.}, title = {Quantum sensing}, journal = {Rev. Mod. Phys.}, publisher = {American Physical Society}, year = {2017}, volume = {89}, pages = {035002}, doi = {10.1103/RevModPhys.89.035002} } |
|
Phys. Rev. B 95, 195308 (2017) |
|
Abstract: Precise knowledge of a quantum system's Hamiltonian is a critical pre-requisite for its use in many quantum information technologies. Here, we report a method for the precise characterization of the nonsecular part of the excited-state Hamiltonian of an electronic-nuclear spin system in diamond. The method relies on the investigation of the dynamic nuclear polarization mediated by the electronic spin, which is currently exploited as a primary tool for initializing nuclear qubits and performing enhanced nuclear magnetic resonance. By measuring the temporal evolution of the population of the ground-state hyperfine levels of a nitrogen-vacancy center, we obtain the first direct estimation of the excited-state transverse hyperfine coupling between its electronic and nitrogen nuclear spin. Our method could also be applied to other electron-nuclear spin systems, such as those related to defects in silicon carbide. | |
BibTeX:
@article{Poggiali17, author = {Poggiali, F. and Cappellaro, P. and Fabbri, N.}, title = {Measurement of the excited-state transverse hyperfine coupling in NV centers via dynamic nuclear polarization}, journal = {Phys. Rev. B}, year = {2017}, volume = {95}, number = {19}, pages = {195308}, doi = {10.1103/PhysRevB.95.195308} } |
|
2016 | UP ↑ |
Conference on Lasers and Electro-Optics In Conference on Lasers and Electro-Optics , FTu3D.1 (2016) |
|
Abstract: Silicon-vacancy (SiV) centers in diamond are bright sources of indistinguishable single photons. We report fabrication of nanowires coupled to single SiV by deterministic ion implantation, yielding greatly enhanced light coupling compared to SiV in bulk. | |
BibTeX:
@inproceedings{Marseglia16, author = {Luca Marseglia and Kasturi Saha and Ashok Ajoy and Tim Schroder and Dirk R. Englund and Tokuyuki TERAJI and junichi isoya and Fedor Jelezko and Ronald Walsworth and Jose L. Pacheco and Daniel Perry and Edward Bielejec and Paola Cappellaro}, title = {A bright nanowire single photon source}, booktitle = {Conference on Lasers and Electro-Optics}, journal = {Conference on Lasers and Electro-Optics}, publisher = {Optical Society of America}, year = {2016}, pages = {FTu3D.1}, doi = {10.1364/CLEO_QELS.2016.FTu3D.1} } |
|
Thesis at: Massachusetts Institute of Technology, (2016) |
|
Abstract: This thesis describes experimental and theoretical work making contributions in the general areas of quantum metrology, simulation and control. Specifically, we describe new approaches for high resolution magnetic resonance imaging using quantum sensors, that could potentially achieve the determination of single molecular structure. We show experiments that boost the sensing resolution of these sensors by over a factor of 100. We also develop separate methods for the sensitive detection of DC magnetic fields, and rotations. Also developed are techniques for the engineering of many-body Hamiltonians with restricted just global control fields, a task of wide interest for quantum simulation. Finally the toolbox available for quantum control is expanded for various applications in quantum information processing and simulation. |
|
BibTeX:
@phdthesis{Ajoy16t, author = {Ajoy, Ashok}, title = {Quantum Assisted Sensing, Simulation and Control}, school = {Massachusetts Institute of Technology}, year = {2016} } |
|
Thesis at: Massachusetts Institute of Technology, (2016) |
|
Abstract: This thesis introduces and experimentally demonstrates coherent control techniques to exploit electron spins in diamond for applications in quantum information processing and quantum sensing. Specifically, optically-detected magnetic double resonance measurements are performed on quantum states of single and multiple electron spins associated with nitrogen-vacancy centers and paramagnetic centers in synthetic diamond crystals. The Walsh reconstruction method is introduced as a general framework to estimate the parameters of deterministic and stochastic time-varying fields with quantum sensors. The Walsh method generalizes sampling techniques based on dynamical decoupling sequences and enables measuring the temporal profile of time-varying magnetic fields with increased precision in the presence of noise and environmental fluctuations. Coherent control techniques are further introduced to identify, integrate, and exploit unknown quantum systems located in the environment of a quantum probe. In particular, entangled states of two and three electron spins in diamond are created to estimate the amplitude of time-varying magnetic fields. These results demonstrate a scalable approach to measure time-varying fields with quantum probes in solid-state materials for applications in environment-assisted quantum metrology, such as real-time functional imaging of neural activity at the level of a single neuron, magnetic resonance spectroscopy and imaging of biological complexes in living cells; and characterization of the structure and dynamics of new magnetic materials. |
|
BibTeX:
@phdthesis{Cooper16t, author = {Cooper-Roy, Alexandre}, title = {Coherent control of electron spins in diamond for quantum information science and quantum sensing}, school = {Massachusetts Institute of Technology}, year = {2016} } |
|
Nature 532, 77-80 (2016) |
|
Abstract: Engineering desired operations on qubits subjected to the deleterious effects of their environment is a critical task in quantum information processing, quantum simulation and sensing. The most common approach relies on open-loop quantum control techniques, including optimal-control algorithms based on analytical or numerical solutions, Lyapunov design3 and Hamiltonian engineering. An alternative strategy, inspired by the success of classical control, is feedback contro. Because of the complications introduced by quantum measurement, closed-loop control is less pervasive in the quantum setting and, with exceptions, its experimental implementations have been mainly limited to quantum optics experiments. Here we implement a feedback-control algorithm using a solid-state spin qubit system associated with the nitrogen vacancy centre in diamond, using coherent feedback to overcome the limitations of measurement-based feedback, and show that it can protect the qubit against intrinsic dephasing noise for milliseconds. In coherent feedback, the quantum system is connected to an auxiliary quantum controller (ancilla) that acquires information about the output state of the system (by an entangling operation) and performs an appropriate feedback action (by a conditional gate). In contrast to open-loop dynamical decoupling techniques, feedback control can protect the qubit even against Markovian noise and for an arbitrary period of time (limited only by the coherence time of the ancilla), while allowing gate operations. It is thus more closely related to quantum error-correction schemes, although these require larger and increasing qubit overheads. Increasing the number of fresh ancillas enables protection beyond their coherence time. We further evaluate the robustness of the feedback protocol, which could be applied to quantum computation and sensing, by exploring a trade-off between information gain and decoherence protection, as measurement of the ancilla-qubit correlation after the feedback algorithm voids the protection, even if the rest of the dynamics is unchanged. | |
BibTeX:
@article{Hirose16, author = {Hirose, Masashi and Cappellaro, Paola}, title = {Coherent feedback control of a single qubit in diamond}, journal = {Nature}, year = {2016}, volume = {532}, number = {7597}, pages = {77--80}, doi = {10.1038/nature17404} } |
|
Phys. Rev. B 93, 045425 (2016) |
|
Abstract: We demonstrate a robust experimental method for determining the depth of individual shallow nitrogen-vacancy (NV) centers in diamond with ~1nm uncertainty. We use a confocal microscope to observe single NV centers and detect the proton nuclear magnetic resonance (NMR) signal produced by objective immersion oil, which has well understood nuclear spin properties, on the diamond surface. We determine the NV center depth by analyzing the NV NMR data using a model that describes the interaction of a single NV center with the statistically polarized proton spin bath. We repeat this procedure for a large number of individual, shallow NV centers and compare the resulting NV depths to the mean value expected from simulations of the ion implantation process used to create the NV centers, with reasonable agreement. | |
BibTeX:
@article{Pham16, author = {Pham, Linh M. and DeVience, Stephen J. and Casola, Francesco and Lovchinsky, Igor and Sushkov, Alexander O. and Bersin, Eric and Lee, Junghyun and Urbach, Elana and Cappellaro, Paola and Park, Hongkun and Yacoby, Amir and Lukin, Mikhail and Walsworth, Ronald L.}, title = {NMR technique for determining the depth of shallow nitrogen-vacancy centers in diamond}, journal = {Phys. Rev. B}, publisher = {American Physical Society}, year = {2016}, volume = {93}, pages = {045425}, doi = {10.1103/PhysRevB.93.045425} } |
|
2015 | UP ↑ |
Phys. Rev. B 92, 020101 (2015) |
|
Abstract: Precise characterization of a system's Hamiltonian is crucial to its high-fidelity control that would enable many quantum technologies, ranging from quantum computation to communication and sensing. In particular, non-secular parts of the Hamiltonian are usually more difficult to characterize, even if they can give rise to subtle but non-negligible effects. Here we present a strategy for the precise estimation of the transverse hyperfine coupling between an electronic and a nuclear spin, exploiting effects due to forbidden transitions during the Rabi driving of the nuclear spin. We applied the method to precisely determine the transverse coupling between a Nitrogen-Vacancy center electronic spin and its Nitrogen nuclear spin. In addition, we show how this transverse hyperfine, that has been often neglected in experiments, is crucial to achieving large enhancements of the nuclear Rabi driving. | |
BibTeX:
@article{Chen15, author = {Chen, Mo and Hirose, Masashi and Cappellaro, Paola}, title = {Measurement of transverse hyperfine interaction by forbidden transitions}, journal = {Phys. Rev. B}, publisher = {American Physical Society}, year = {2015}, volume = {92}, pages = {020101}, doi = {10.1103/PhysRevB.92.020101} } |
|
Nat Nano 10, 859-864 (2015) |
|
Abstract: Optically detected magnetic resonance using nitrogen?vacancy (NV) colour centres in diamond is a leading modality for nanoscale magnetic field imaging, as it provides single electron spin sensitivity, three-dimensional resolution better than 1?nm and applicability to a wide range of physical and biological, samples under ambient conditions. To date, however, NV-diamond magnetic imaging has been performed using 'real-space' techniques, which are either limited by optical diffraction to ~250?nm resolution or require slow, point-by-point scanning for nanoscale resolution, for example, using an atomic force microscope, magnetic tip, or super-resolution optical imaging. Here, we introduce an alternative technique of Fourier magnetic imaging using NV-diamond. In analogy with conventional magnetic resonance imaging (MRI), we employ pulsed magnetic field gradients to phase-encode spatial information on NV electronic spins in wavenumber or 'k-space' followed by a fast Fourier transform to yield real-space images with nanoscale resolution, wide field of view and compressed sensing speed-up. | |
BibTeX:
@article{Arai15, author = {Arai, K. and Belthangady, C. and Zhang, H. and Bar-Gill, N. and DeVience, S.J. and Cappellaro, P. and Yacoby, A. and Walsworth, R.L.}, title = {Fourier magnetic imaging with nanoscale resolution and compressed sensing speed-up using electronic spins in diamond}, journal = {Nat Nano}, publisher = {Nature Publishing Group}, year = {2015}, volume = {10}, pages = {859--864} } |
|
Quantum Information Processing 14, 3233 (2015) |
|
Abstract: We present an algebraic framework to study the time-optimal synthesis of arbitrary unitaries in SU(2), when the control set is restricted to rotations around two non-parallel axes in the Bloch sphere. Our method bypasses commonly used control-theoretical techniques and easily imposes necessary conditions on time-optimal sequences. In a straightforward fashion, we prove that time-optimal sequences are solely parametrized by three rotation angles and derive general bounds on those angles as a function of the relative rotation speed of each control and the angle between the axes. Results are substantially different whether both clockwise and counterclockwise rotations about the given axes are allowed, or only clockwise rotations. In the first case, we prove that any finite time-optimal sequence is composed at most of five control concatenations, while for the more restrictive case, we present scaling laws on the maximum length of any finite time-optimal sequence. The bounds we find for both cases are stricter than previously published ones and severely constrain the structure of time-optimal sequences, allowing for an efficient numerical search of the time-optimal solution. Our results can be used to find the time-optimal evolution of qubit systems under the action of the considered control set and thus potentially increase the number of realizable unitaries before decoherence. | |
BibTeX:
@article{Aiello15q, author = {Aiello, ClariceD. and Allegra, Michele and Hemmerling, Boerge and Wan, Xiaoting and Cappellaro, Paola}, title = {Algebraic synthesis of time-optimal unitaries in SU(2) with alternating controls}, journal = {Quantum Information Processing}, publisher = {Springer US}, year = {2015}, volume = {14} pages = {3233}, doi = {10.1007/s11128-015-1045-6} } |
|
Physics , 56 (2015) |
|
Abstract: An optical technique polarizes the spin of nuclei in silicon carbide, offering a potential new route to nuclear spin-based quantum memory. A Viewpoint on: Optical Polarization of Nuclear Spins in Silicon Carbide Abram L. Falk, Paul V. Klimov, Viktor Ivady, Krisztian Szasz, David J. Christle, William F. Koehl, Adam Gali, and, and David D. Awschalom Physical Review Letters 114, 247603 2015 |
|
BibTeX:
@article{Cappellaro15, author = {Cappellaro, P.}, title = {Polarizing Nuclear Spins in Silicon Carbide}, journal = {Physics}, year = {2015}, number = {8}, pages = {56}, doi = {10.1103/Physics.8.56} } |
|
Phys. Rev. X 5, 011001 (2015) |
|
Abstract: Nuclear spin imaging at the atomic level is essential for the understanding of fundamental biological phenomena and for applications such as drug discovery. The advent of novel nanoscale sensors promises to achieve the long-standing goal of single-protein, high spatial-resolution structure determination under ambient conditions. In particular, quantum sensors based on the spin-dependent photoluminescence of nitrogen-vacancy (NV) centers in diamond have recently been used to detect nanoscale ensembles of external nuclear spins. While NV sensitivity is approaching single-spin levels, extracting relevant information from a very complex structure is a further challenge since it requires not only the ability to sense the magnetic field of an isolated nuclear spin but also to achieve atomic-scale spatial resolution. Here, we propose a method that, by exploiting the coupling of the NV center to an intrinsic quantum memory associated with the nitrogen nuclear spin, can reach a tenfold improvement in spatial resolution, down to atomic scales. The spatial resolution enhancement is achieved through coherent control of the sensor spin, which creates a dynamic frequency filter selecting only a few nuclear spins at a time. We propose and analyze a protocol that would allow not only sensing individual spins in a complex biomolecule, but also unraveling couplings among them, thus elucidating local characteristics of the molecule structure. | |
BibTeX:
@article{Ajoy15, author = {Ajoy, A. and Bissbort, U. and Lukin, M.D. and Walsworth, R.L. and Cappellaro, P.}, title = {Atomic-Scale Nuclear Spin Imaging Using Quantum-Assisted Sensors in Diamond}, journal = {Phys. Rev. X}, publisher = {American Physical Society}, year = {2015}, volume = {5}, pages = {011001}, doi = {10.1103/PhysRevX.5.011001} } |
|
Phys. Rev. A 91, 042340 (2015) |
|
Abstract: Indirect control of qubits by a quantum actuator has been proposed as an appealing strategy to manipulate qubits that couple only weakly to external fields. While universal quantum control can be easily achieved when the actuator-qubit coupling is anisotropic, the efficiency of this approach is less clear. Here we analyze the time efficiency of quantum actuator control. We describe a strategy to find time-optimal control sequences by the quantum actuator and compare their gate times with direct driving, identifying regimes where the actuator control performs faster. As a paradigmatic example, we focus on a specific implementation based on the nitrogen-vacancy center electronic spin in diamond (the actuator) and nearby C13 nuclear spins (the qubits). | |
BibTeX:
@article{Aiello15, author = {Aiello, Clarice D. and Cappellaro, Paola}, title = {Time-optimal control by a quantum actuator}, journal = {Phys. Rev. A}, publisher = {American Physical Society}, year = {2015}, volume = {91}, pages = {042340}, doi = {10.1103/PhysRevA.91.042340} } |
|
Thesis at: Massachusetts Institute of Technology, Department of Nuclear Science and Engineering (2015) |
|
Abstract: The precise control of a system which behaves according to the principles of quantum mechanics is an indispensable task in order to fully harness unique properties of quantum mechanics, such as superposition and entanglement, for practical applications. Leveraging the quantum nature of the system would enable for example the implementation of quantum computation and quantum metrology. However, any realistic quantum system is inevitably coupled to its environment. The interaction with its surroundings irrevocably destroys the quantum nature of the system: mitigating decoherence is thus one of the central problems in quantum control. In this thesis, we develop novel control methods to protect a qubit from decoherence by two distinct approaches and demonstrate them experimentally using the nitrogen-vacancy (NV) center in diamond. The first method rests on an open-loop control scheme and it is tailored to improve quantum sensing tasks. We develop a continuous dynamical decoupling (CoDD) method that allows us to tune the degree of protection from a dephasing environment. Exploiting this flexibility, we show that the CoDD can be used to measure magnetic fields with sensitivity comparable to existing methods, while providing superior versatility in practical experimental settings. This protocol can adapt to various sensing conditions, such as measurement time and sensitive frequency, that might occur in biological and material science. The second method exploits a coherent feedback protocol. We take advantage of a long-lived nuclear spin as an ancillary spin to protect the qubit of interest from decoherence. We show that the protocol protects the qubit as long as open-loop dynamical decoupling control schemes and it can be used against more general types of noise than the open-loop protocol. This method thus offers an alternative protocol to protect the qubit from decoherence in quantum computation and quantum metrology. |
|
BibTeX:
@phdthesis{Hirose15t, author = {Hirose, Masashi}, title = {Quantum Control of Spin Systems in diamond}, school = {Massachusetts Institute of Technology}, year = {2015} } |
|
B.S. Thesis at: Massachusetts Institute of Technology, Department of Nuclear Science & Engineering (2015) |
|
Abstract In this thesis, we discuss two problems of quantum dynamics in the presence of alternating controls. Alternating controls arise in many protocols designed to extend the duration over which a qubit is a useful computational resource. This is accomplished by control sequences that either retard decoherence, or that accomplish a quantum operation in as short a time as possible. The first problem tackles the use of a composite-pulse control sequence known as 'rotary-echo' for quantum magnetometry purposes. The sequence consists in the continuous drive of a qubit, with field phases that alternate at specific intervals. We implement such a magnetometry protocol using an electronic qubit in diamond, and experimentally confirm the flexibility yielded by the tuning of sequence parameters that achieves a good compromise between decoherence resilience and sensitivity. The second problem theoretically investigates the time-optimal evolution of a qubit in the case of a restricted control set composed of alternating rotations around two non-parallel axes on the Bloch sphere. Using accessible algebraic methods, we show that experimental parameters, such as the angle between the two rotation axes, restrict the necessary structure of time-optimal sequences. We propose to implement such an evolution through alternate driving as an advantageous alternative to the slow, noisy direct addressing of a nuclear qubit anisotropically hyperfine-coupled to an electronic spin in diamond. | |
BibTeX:
@phdthesis{Lopez15t, author = {Nicolas Lopez}, title = {All-Optical Method of Nanoscale Magnetometry for Ensembles of Nitrogen-Vacancy Defects in Diamond}, school = {Massachusetts Institute of Technology}, year = {2014} } |
|
2014 | UP ↑ |
Nature Comms. 5, 3141 (2014) |
|
Abstract: Quantum probes enable the sensitive detection of time-varying fields with high spatial resolution, opening the possibility to explore biological functions as well as materials and physical phenomena at the nanometer scale. In particular, nitrogen-vacancy (NV) centers in diamond have recently emerged as promising sensors of magnetic and electric fields. Although coherent control techniques have measured the amplitude of constant or oscillating fields, these techniques are unable to measure time-varying fields with unknown dynamics. Here we introduce a coherent acquisition method to accurately reconstruct the arbitrary profile of time-varying fields using coherent control sequences associated with the Walsh functions. These sequences act as digital filters that efficiently extract information about the dynamics of the field while suppressing decoherence. We experimentally demonstrate the Walsh reconstruction method by performing proof-of-principle reconstruction of the magnetic field radiated by a physical model of a neuron using a single electronic spin in diamond. These results will be useful for performing time-resolved magnetic sensing with quantum probes in a broad array of physical and biological systems at the nanometer scale. | |
BibTeX:
@article{Cooper14, author = {Cooper, A. and Magesan, E. and Yum, H.N. and Cappellaro, P.}, title = {Time-resolved magnetic sensing with electronic spins in diamond}, journal = {Nature Comms.}, year = {2014}, volume = {5}, pages = {3141}, doi = {10.1038/ncomms4141} } |
|
In Quantum State Transfer and Network Engineering , 183-222 (2014) |
|
Abstract: Nuclear spin systems and magnetic resonance techniques have provided a fertile platform for experimental investigation of quantum state transfer in spin chains. From the first observation of polarization transfer, predating the formal definition of quantum state transfer, to the realization of state transfer simulations in small molecules and in larger solid-state spin systems, the experiments have drawn on the strengths of nuclear magnetic resonance (NMR), in particular on its long history of well-developed control techniques. NMR implementations have been invaluable both as proof-of-principle demonstrations of quantum state transfer protocols and to explore dynamics occurring in real systems that go beyond what can be analytically solved or numerically simulated. In addition, control techniques developed in these systems to engineer the Hamiltonians required for transport can be adopted in potentially scalable quantum information processing architectures. In this contribution we describe recent results and outline future directions of research in magnetic-resonance based implementation of quantum state transfer in spin chains. | |
BibTeX:
@incollection{Cappellaro14, author = {Cappellaro, Paola}, editor = {Nikolopoulos, Georgios M. and Jex, Igor}, title = {Implementation of State Transfer Hamiltonians in Spin Chains with Magnetic Resonance Techniques}, booktitle = {Quantum State Transfer and Network Engineering}, publisher = {Springer Berlin Heidelberg}, year = {2014}, pages = {183-222}, doi = {10.1007/978-3-642-39937-4_6} } |
|
Thesis at: Massachusetts Institute of Technology, Department of Electrical Engineering & Computer Science and Engineering (2014) |
|
Abstract In this thesis, we discuss two problems of quantum dynamics in the presence of alternating controls. Alternating controls arise in many protocols designed to extend the duration over which a qubit is a useful computational resource. This is accomplished by control sequences that either retard decoherence, or that accomplish a quantum operation in as short a time as possible. The first problem tackles the use of a composite-pulse control sequence known as 'rotary-echo' for quantum magnetometry purposes. The sequence consists in the continuous drive of a qubit, with field phases that alternate at specific intervals. We implement such a magnetometry protocol using an electronic qubit in diamond, and experimentally confirm the flexibility yielded by the tuning of sequence parameters that achieves a good compromise between decoherence resilience and sensitivity. The second problem theoretically investigates the time-optimal evolution of a qubit in the case of a restricted control set composed of alternating rotations around two non-parallel axes on the Bloch sphere. Using accessible algebraic methods, we show that experimental parameters, such as the angle between the two rotation axes, restrict the necessary structure of time-optimal sequences. We propose to implement such an evolution through alternate driving as an advantageous alternative to the slow, noisy direct addressing of a nuclear qubit anisotropically hyperfine-coupled to an electronic spin in diamond. | |
BibTeX:
@phdthesis{Aiello14t, author = {Clarice D. Aiello}, title = {Qubit dynamics under alternating controls}, school = {Massachusetts Institute of Technology}, year = {2014} } | |
2013 | UP ↑ |
Phys. Rev A 88, 062109 (2013) |
|
Abstract: We present methods that can provide an exponential savings in the resources required to perform dynamic parameter estimation using quantum systems. The key idea is to merge classical compressive sensing techniques with quantum control methods to efficiently estimate time-dependent parameters in the system Hamiltonian. We show that incoherent measurement bases and, more generally, suitable random measurement matrices can be created by performing simple control sequences on the quantum system. Since random measurement matrices satisfying the restricted isometry property can be used to reconstruct any sparse signal in an efficient manner, and many physical processes are approximately sparse in some basis, these methods can potentially be useful in a variety of applications such as quantum sensing and magnetometry. We illustrate the theoretical results throughout the presentation with various practically relevant numerical examples. | |
BibTeX: @article{Magesan13c, author = {Magesan, E. and Cooper, A and Yum, H.N. and Cappellaro, P.}, title = {Compressing measurements in quantum dynamic parameter estimation}, journal = {Phys. Rev. A}, abstract = {We present methods that can provide an exponential savings in the resources required to perform dynamic parameter estimation using quantum systems. The key idea is to merge classical compressive sensing techniques with quantum control methods to efficiently estimate time-dependent parameters in the system Hamiltonian. We show that incoherent measurement bases and, more generally, suitable random measurement matrices can be created by performing simple control sequences on the quantum system. Since random measurement matrices satisfying the restricted isometry property can be used to reconstruct any sparse signal in an efficient manner, and many physical processes are approximately sparse in some basis, these methods can potentially be useful in a variety of applications such as quantum sensing and magnetometry. We illustrate the theoretical results throughout the presentation with various practically relevant numerical examples.}, year = {2013}, volume = {88}, pages = {062109}, doi = {10.1103/PhysRevA.88.062109}, url={http://link.aps.org/doi/10.1103/PhysRevA.88.062109} } | |
Nat. Commun. 4, 1419- (2013) |
|
Abstract: The sensitivity of quantum magnetometer is challenged by control errors and, especially in the solid state, by their short coherence times. Refocusing techniques can overcome these limitations and improve the sensitivity to periodic fields, but they come at the cost of reduced bandwidth and cannot be applied to sense static or aperiodic fields. Here we experimentally demonstrate that continuous driving of the sensor spin by a composite pulse known as rotary-echo yields a flexible magnetometry scheme, mitigating both driving power imperfections and decoherence. A suitable choice of rotary-echo parameters compensates for different scenarios of noise strength and origin. The method can be applied to nanoscale sensing in variable environments or to realize noise spectroscopy. In a room-temperature implementation, based on a single electronic spin in diamond, composite-pulse magnetometry provides a tunable trade-off between sensitivities in the mTHz^1/2 range, comparable with those obtained with Ramsey spectroscopy, and coherence times approaching T1. | |
BibTeX:
@article{Aiello13, author = {Aiello, Clarice D. and Hirose, Masashi and Cappellaro, Paola}, title = {Composite-pulse magnetometry with a solid-state quantum sensor}, journal = {Nat. Commun.}, publisher = {Nat Publishing Group, a division of Macmillan Publishers Limited. All Rights Reserved.}, year = {2013}, volume = {4}, pages = {1419--}, doi = {10.1038/ncomms2375} } |
|
Phys. Rev. B 87, 064303 (2013) |
|
Abstract: Spin chains have been proposed as wires to transport information between distributed registers in a quantum information processor. Unfortunately, the challenges in manufacturing linear chains with engineered couplings has hindered experimental implementations. Here we present strategies to achieve perfect quantum information transport in arbitrary spin networks. Our proposal is based on the weak coupling limit for pure state transport, where information is transferred between two end spins that are only weakly coupled to the rest of the network. This regime allows ignoring the complex, internal dynamics of the bulk network and relying on virtual transitions or on the coupling to a single bulk eigenmode. We further introduce control methods capable of tuning the transport process and achieve perfect fidelity with limited resources, involving only manipulation of the end qubits. These strategies could be thus applied not only to engineered systems with relaxed fabrication precision, but also to naturally occurring networks; specifically, we discuss the practical implementation of quantum state transfer between two separated nitrogen vacancy (NV) centers through a network of nitrogen substitutional impurities. | |
BibTeX:
@article{Ajoy13, author = {Ajoy, Ashok and Cappellaro, Paola}, title = {Perfect quantum transport in arbitrary spin networks}, journal = {Phys. Rev. B}, year = {2013}, volume = {87}, pages = {064303}, doi = {10.1103/PhysRevB.87.064303} } |
|
Phys. Rev. Lett. 110, 220503 (2013) |
|
Abstract: We propose a method for Hamiltonian engineering that requires no local control but only relies on collective qubit rotations and field gradients. The technique achieves a spatial modulation of the coupling strengths via a dynamical construction of a weighting function combined with a Bragg grating. As an example, we demonstrate how to generate the ideal Hamiltonian for perfect quantum information transport between two separated nodes of a large spin network. We engineer a spin chain with optimal couplings starting from a large spin network, such as one naturally occurring in crystals, while decoupling all unwanted interactions. For realistic experimental parameters, our method can be used to drive almost perfect quantum information transport at room temperature. The Hamiltonian engineering method can be made more robust under decoherence and coupling disorder by a novel apodization scheme. Thus, the method is quite general and can be used to engineer the Hamiltonian of many complex spin lattices with different topologies and interactions. | |
BibTeX:
@article{Ajoy13l, author = {Ajoy, A. and Cappellaro, P.}, title = {Quantum simulation via filtered Hamiltonian engineering: application to perfect quantum transport in spin networks}, journal = {Phys. Rev. Lett.}, year = {2013}, volume = {110}, pages = {220503}, doi = {10.1103/PhysRevLett.110.220503} } |
|
Phys. Rev. Lett. 110, 157601 (2013) |
|
Abstract: Under ambient conditions, spin impurities in solid-state systems are found in thermally mixed states and are optically "dark"; i.e., the spin states cannot be optically controlled. Nitrogen-vacancy (NV) centers in diamond are an exception in that the electronic spin states are "bright"; i.e., they can be polarized by optical pumping, coherently manipulated with spin-resonance techniques, and read out optically, all at room temperature. Here we demonstrate a scheme to resonantly couple bright NV electronic spins to dark substitutional-nitrogen (P1) electronic spins by dressing their spin states with oscillating magnetic fields. This resonant coupling mechanism can be used to transfer spin polarization from NV spins to nearby dark spins and could be used to cool a mesoscopic bath of dark spins to near-zero temperature, thus providing a resource for quantum information and sensing, and aiding studies of quantum effects in many-body spin systems. | |
BibTeX:
@article{Belthangady13, author = {Belthangady, C. and Bar-Gill, N. and Pham, L. M. and Arai, K. and Le Sage, D. and Cappellaro, P. and Walsworth, R. L.}, title = {Dressed-State Resonant Coupling between Bright and Dark Spins in Diamond}, journal = {Phys. Rev. Lett.}, year = {2013}, volume = {110}, pages = {157601}, doi = {10.1103/PhysRevLett.110.157601} } |
|
New J. Phys. 15, 093035 (2013) |
|
Abstract: Strategies to protect multi-qubit states against decoherence are difficult to formulate because of their complex many-body dynamics. A better knowledge of the decay dynamics would help in the construction of dynamical decoupling control schemes. Here we use solid-state nuclear magnetic resonance techniques to experimentally investigate decay of coherent multi-spin states in linear spin chains. Leveraging on the quasi-one-dimension geometry of fluorapatite crystal spin systems, we can gain a deeper insight on the multi-spin states created by the coherent evolution, and their subsequent decay, than it is possible in three-dimensional (3D) systems. We are then able to formulate an analytical model that captures the key features of the decay. We can thus compare the decoherence behavior for different initial states of the spin chain and link their decay rate to the state characteristics, in particular their coherence and long-range correlation among spins. Our experimental and theoretical study shows that the spin chains undergo a rich dynamics, with a slower decay rate than for the 3D case, and thus might be more amenable to decoupling techniques. | |
BibTeX:
@article{Kaur13, author = {G Kaur and A Ajoy and P Cappellaro}, title = {Decay of spin coherences in one-dimensional spin systems}, journal = {New J. Phys.}, year = {2013}, volume = {15}, number = {9}, pages = {093035}, doi = {10.1088/1367-2630/15/9/093035} } |
|
Phys. Rev. A 88, 032107 (2013) |
|
Abstract: Quantum systems have shown great promise for precision metrology thanks to advances in their control. This has allowed not only the sensitive estimation of external parameters but also the reconstruction of their temporal profile. In particular, quantum control techniques and orthogonal function theory have been applied to the reconstruction of the complete profiles of time-varying magnetic fields. Here, we provide a detailed theoretical analysis of the reconstruction method based on the Walsh functions, highlighting the relationship between the orthonormal Walsh basis, sensitivity of field reconstructions, data compression techniques, and dynamical decoupling theory. Specifically, we show how properties of the Walsh basis and a detailed sensitivity analysis of the reconstruction protocol provide a method to characterize the error between the reconstructed and true fields. In addition, we prove various results about the negligibility function on binary sequences which lead to data compression techniques in the Walsh basis and a more resource-efficient reconstruction protocol. The negligibility proves a fruitful concept to unify the information content of Walsh functions and their dynamical decoupling power, which makes the reconstruction method robust against noise. | |
BibTeX:
@article{Magesan13, author = {Magesan, Easwar and Cooper, Alexandre and Yum, Honam and Cappellaro, Paola}, title = {Reconstructing the profile of time-varying magnetic fields with quantum sensors}, journal = {Phys. Rev. A}, year = {2013}, volume = {88}, pages = {032107}, doi = {10.1103/PhysRevA.88.032107} } |
|
Phys. Rev. A 88, 022127 (2013) |
|
Abstract: Efficient methods for characterizing the performance of quantum measurements are important in the experimental quantum sciences. Ideally, one requires both a physically relevant distinguishability measure between measurement operations and a well-defined experimental procedure for estimating the distinguishability measure. Here, we propose the average measurement fidelity and error between quantum measurements as distinguishability measures. We present protocols for obtaining bounds on these quantities that are both estimable using experimentally accessible quantities and scalable in the size of the quantum system. We also explain why the bounds should be valid in large generality and illustrate the method via numerical examples. | |
BibTeX:
@article{Magesan13a, author = {Magesan, Easwar and Cappellaro, Paola}, title = {Experimentally efficient methods for estimating the performance of quantum measurements}, journal = {Phys. Rev. A}, year = {2013}, volume = {88}, pages = {022127}, doi = {10.1103/PhysRevA.88.022127} } |
|
2012 | UP ↑ |
Phys. Rev. A 85, 042305 (2012) |
|
Abstract: Quantum spin networks can be used to transport information between separated registers in a quantum-information processor. To find a practical implementation, the strict requirements of ideal models for perfect state transfer need to be relaxed, allowing for complex coupling topologies and general initial states. Here we analyze transport in complex quantum spin networks in the maximally mixed state and derive explicit conditions that should be satisfied by propagators for perfect state transport. Using a description of the transport process as a quantum walk over the network, we show that it is necessary to phase-correlate the transport processes occurring along all the possible paths in the network. We provide a Hamiltonian that achieves this correlation and use it in a constructive method to derive engineered couplings for perfect transport in complicated network topologies. | |
BibTeX:
@article{Ajoy12, author = {Ajoy, Ashok and Cappellaro, Paola}, title = {Mixed-state quantum transport in correlated spin networks}, journal = {Phys. Rev. A}, year = {2012}, volume = {85}, pages = {042305}, doi = {10.1103/PhysRevA.85.042305} } |
|
Phys. Rev. A 86, 062104 (2012) |
|
Abstract: Gyroscopes find wide applications in everyday life from navigation and inertial sensing to rotation sensors in hand-held devices and automobiles. Current devices, based on either atomic or solid-state systems, impose a choice between long-time stability and high sensitivity in a miniaturized system. Here, we introduce a quantum sensor that overcomes these limitations by providing a sensitive and stable three-axis gyroscope in the solid state. We achieve high sensitivity by exploiting the long coherence time of the 14N nuclear spin associated with the nitrogen-vacancy center in diamond, combined with the efficient polarization and measurement of its electronic spin. Although the gyroscope is based on a simple Ramsey interferometry scheme, we use coherent control of the quantum sensor to improve its coherence time and robustness against long-time drifts. Such a sensor can achieve a sensitivity of eta~0.5 (mdeg s-1)/Root Hz mm3 while offering enhanced stability in a small footprint. In addition, we exploit the four axes of delocalization of the nitrogen-vacancy center to measure not only the rate of rotation, but also its direction, thus obtaining a compact three-axis gyroscope. | |
BibTeX:
@article{Ajoy12g, author = {Ajoy, Ashok and Cappellaro, Paola}, title = {Stable three-axis nuclear-spin gyroscope in diamond}, journal = {Phys. Rev. A}, year = {2012}, volume = {86}, pages = {062104}, doi = {10.1103/PhysRevA.86.062104} } |
|
Nat Commun. 3, 858 (2012) |
|
Abstract: Multi-qubit systems are crucial for the advancement and application of quantum science. Such systems require maintaining long coherence times while increasing the number of qubits available for coherent manipulation. For solid-state spin systems, qubit coherence is closely related to fundamental questions of many-body spin dynamics. Here we apply a coherent spectroscopic technique to characterize the dynamics of the composite solid-state spin environment of nitrogen-vacancy colour centres in room temperature diamond. We identify a possible new mechanism in diamond for suppression of electronic spin-bath dynamics in the presence of a nuclear spin bath of sufficient concentration. This suppression enhances the efficacy of dynamical decoupling techniques, resulting in increased coherence times for multi-spin-qubit systems, thus paving the way for applications in quantum information, sensing and metrology. | |
BibTeX:
@article{Bar-Gill12, author = {Bar-Gill, N. and Pham, L.M. and Belthangady, C. and Le Sage, D. and Cappellaro, P. and Maze, J.R. and Lukin, M.D. and Yacoby, A. and Walsworth, R.}, title = {Suppression of spin-bath dynamics for improved coherence of multi-spin-qubit systems}, journal = {Nat Commun.}, year = {2012}, volume = {3}, pages = {858}, doi = {10.1038/ncomms1856} } |
|
Phys. Rev. A 85, 030301(R) (2012) |
|
Abstract: We present a measurement scheme capable of achieving the quantum limit of parameter estimation using an adaptive strategy that minimizes the parameter's variance at each step. The adaptive rule we propose makes the scheme robust against errors, in particular imperfect readouts, a critical requirement to extend adaptive schemes from quantum optics to solid-state sensors. Thanks to recent advances in single-shot readout capabilities for electronic spins in the solid state (such as nitrogen vacancy centers in diamond), this scheme can also be applied to estimate the polarization of a spin bath coupled to the sensor spin. In turns, the measurement process decreases the entropy of the spin bath resulting in longer coherence times of the sensor spin. | |
BibTeX:
@article{Cappellaro12, author = {Cappellaro, Paola}, title = {Spin-bath narrowing with adaptive parameter estimation}, journal = {Phys. Rev. A}, year = {2012}, volume = {85}, pages = {030301(R)}, doi = {10.1103/PhysRevA.85.030301} } |
|
Phys. Rev. A 85, 032336 (2012) |
|
Abstract: We investigate the sensitivity of a recently proposed method for precision measurement [ Phys. Rev. Lett. 106 140502 (2011)], focusing on an implementation based on solid-state spin systems. The scheme amplifies a quantum sensor response to weak external fields by exploiting its coupling to spin impurities in the environment. We analyze the limits to the sensitivity due to decoherence and propose dynamical decoupling schemes to increase the spin coherence time. The sensitivity is also limited by the environment spin polarization; therefore, we discuss strategies to polarize the environment spins and present a method to extend the scheme to the case of zero polarization. The coherence time and polarization determine a figure of merit for the environment's ability to enhance the sensitivity compared to echo-based sensing schemes. This figure of merit can be used to engineer optimized samples for high-sensitivity nanoscale magnetic sensing, such as diamond nanocrystals with controlled impurity density. | |
BibTeX:
@article{Cappellaro12a, author = {Cappellaro, P. and Goldstein, G. and Hodges, J. S. and Jiang, L. and Maze, J. R. and Sørensen, A. S. and Lukin, M. D.}, title = {Environment-assisted metrology with spin qubits}, journal = {Phys. Rev. A}, year = {2012}, volume = {85}, pages = {032336}, doi = {10.1103/PhysRevA.85.032336} } |
|
Phys. Rev. A 86, 062320 (2012) |
|
Abstract: Solid-state qubits hold the promise to achieve an unmatched combination of sensitivity and spatial resolution. To achieve their potential, the qubits need, however, to be shielded from the deleterious effects of the environment. While dynamical decoupling techniques can improve the coherence time, they impose a compromise between sensitivity and the frequency range of the field to be measured. Moreover, the performance of pulse sequences is ultimately limited by control bounds and errors. Here we analyze a versatile alternative based on continuous driving. We find that continuous dynamical decoupling schemes can be used for ac magnetometry, providing similar frequency constraints on the ac field and improved sensitivity for some noise regimes. In addition, the flexibility of phase and amplitude modulation could yield superior robustness to driving errors and a better adaptability to external experimental scenarios. | |
BibTeX:
@article{Hirose12, author = {Hirose, Masashi and Aiello, Clarice D. and Cappellaro, Paola}, title = {Continuous dynamical decoupling magnetometry}, journal = {Phys. Rev. A}, year = {2012}, volume = {86}, pages = {062320}, doi = {10.1103/PhysRevA.86.062320} } |
|
New J. Phys. 14, 083005 (2012) |
|
Abstract: Linear chains of spins acting as quantum wires are a promising approach for achieving scalable quantum information processors. Nuclear spins in apatite crystals provide an ideal test bed for the experimental study of quantum information transport, as they closely emulate a one-dimensional spin chain, while magnetic resonance techniques can be used to drive the spin chain dynamics and probe the accompanying transport mechanisms. Here we demonstrate initialization and readout capabilities in these spin chains, even in the absence of single-spin addressability. These control schemes enable preparing desired states for quantum information transport and probing their evolution under the transport Hamiltonian. We further optimize the control schemes by a detailed analysis of 19 F NMR lineshape. | |
BibTeX:
@article{Kaur12, author = {Gurneet Kaur and Paola Cappellaro}, title = {Initialization and readout of spin chains for quantum information transport}, journal = {New J. Phys.}, year = {2012}, volume = {14}, number = {8}, pages = {083005}, doi = {10.1088/1367-2630/14/8/083005} } |
|
Phys. Rev. B 86, 045214 (2012) |
|
Abstract: We use multipulse dynamical decoupling to increase the coherence lifetime (T2) of large numbers of nitrogen-vacancy (NV) electronic spins in room temperature diamond, thus enabling scalable applications of multispin quantum information processing and metrology. We realize an order-of-magnitude extension of the NV multispin T2 in three diamond samples with widely differing spin impurity environments. In particular, for samples with nitrogen impurity concentration ?1 ppm, we extend T2 to >2 ms, comparable to the longest coherence time reported for single NV centers, and demonstrate a tenfold enhancement in NV multispin sensing of ac magnetic fields. | |
BibTeX:
@article{Pham12, author = {Pham, L. M. and Bar-Gill, N. and Belthangady, C. and Le Sage, D. and Cappellaro, P. and Lukin, M. D. and Yacoby, A. and Walsworth, R. L.}, title = {Enhanced solid-state multispin metrology using dynamical decoupling}, journal = {Phys. Rev. B}, year = {2012}, volume = {86}, pages = {045214}, doi = {10.1103/PhysRevB.86.045214} } |
|
IEEE TAC 57, 1931 -1944 (2012) |
|
Abstract: We consider finite-dimensional Markovian open quantum systems, and characterize the extent to which time-independent Hamiltonian control may allow to stabilize a target quantum state or subspace and optimize the resulting convergence speed. For a generic Lindblad master equation, we introduce a dissipation-induced decomposition of the associated Hilbert space, and show how it serves both as a tool to analyze global stability properties for given control resources and as the starting point to synthesize controls that ensure rapid convergence. The resulting design principles are illustrated in realistic Markovian control settings motivated by quantum information processing, including quantum-optical systems and nitrogen-vacancy centers in diamond. | |
BibTeX:
@article{Ticozzi12, author = {Ticozzi, F. and Lucchese, R. and Cappellaro, P. and Viola, L.}, title = {Hamiltonian Control of Quantum Dynamical Semigroups: Stabilization and Convergence Speed}, journal = {IEEE TAC}, year = {2012}, volume = {57}, number = {8}, pages = {1931 -1944}, doi = {10.1109/TAC.2012.2195858} } |
|
2011 | UP ↑ |
Phys. Rev. A 83, 032304 (2011) |
|
Abstract: Spin chains have been proposed as quantum wires in many quantum-information processing architectures. Coherent transmission of quantum information in spin chains over short distances is enabled by their internal dynamics, which drives the transport of single-spin excitations in perfectly polarized chains. Given the practical challenge of preparing the chain in a pure state, we propose to use a chain that is initially in the maximally mixed state. We compare the transport properties of pure and mixed-state chains and find similarities that enable the experimental study of pure-state transfer via mixed-state chains. We also demonstrate protocols for the perfect transfer of quantum information in these chains. Remarkably, mixed-state chains allow the use of Hamiltonians that do not preserve the total number of single-spin excitations and are more readily obtainable from the naturally occurring magnetic dipolar interaction. We discuss experimental implementations using solid-state nuclear magnetic resonance and defect centers in diamond. | |
BibTeX:
@article{Cappellaro11, author = {Cappellaro, Paola and Viola, Lorenza and Ramanathan, Chandrasekhar }, title = {Coherent-state transfer via highly mixed quantum spin chains}, journal = {Phys. Rev. A}, year = {2011}, volume = {83}, number = {3}, pages = {032304}, doi = {10.1103/PhysRevA.83.032304} } |
|
Phys. Rev. Lett. 106, 140502 (2011) |
|
Abstract: We describe a method to enhance the sensitivity of precision measurements that takes advantage of the environment of a quantum sensor to amplify the response of the sensor to weak external perturbations. An individual qubit is used to sense the dynamics of surrounding ancillary qubits, which are in turn affected by the external field to be measured. The resulting sensitivity enhancement is determined by the number of ancillas that are coupled strongly to the sensor qubit; it does not depend on the exact values of the coupling strengths and is resilient to many forms of decoherence. The method achieves nearly Heisenberg-limited precision measurement, using a novel class of entangled states. We discuss specific applications to improve clock sensitivity using trapped ions and magnetic sensing based on electronic spins in diamond. | |
BibTeX:
@article{Goldstein11, author = {Goldstein, G. and Cappellaro, P. and Maze, J.~R. and Hodges, J.~S. and Jiang, L. and Sørensen, A.~S. and Lukin, M.~D.}, title = {Environment Assisted Precision Measurement}, journal = {Phys. Rev. Lett.}, year = {2011}, volume = {106}, number = {14}, pages = {140502}, doi = {10.1103/PhysRevLett.106.140502} } |
|
New J. Phys. 13, 045021 (2011) |
|
Abstract: We demonstrate a method of imaging spatially varying magnetic fields using a thin layer of nitrogen-vacancy (NV) centers at the surface of a diamond chip. Fluorescence emitted by the two-dimensional NV ensemble is detected by a CCD array, from which a vector magnetic field pattern is reconstructed. As a demonstration, ac current is passed through wires placed on the diamond chip surface, and the resulting ac magnetic field patterns are imaged using an echo-based technique with sub-micron resolution over a 140� um 140 um field of view, giving single-pixel sensitivity . We discuss ongoing efforts to further improve the sensitivity, as well as potential bioimaging applications such as real-time imaging of activity in functional, cultured networks of neurons. | |
BibTeX:
@article{Pham11, author = {Pham, L M and Le Sage, D and Stanwix, P L and Yeung, T K and Glenn, D and Trifonov, A and Cappellaro, P and Hemmer, P R and Lukin, M D and Park, H and Yacoby, A and Walsworth, R L}, title = {Magnetic field imaging with nitrogen-vacancy ensembles}, journal = {New J. Phys.}, publisher = {IOP Publishing}, year = {2011}, volume = {13}, number = {4}, pages = {045021}, doi = {10.1088/1367-2630/13/4/045021} } |
|
New J. Phys. 13, 103015 (2011) |
|
Abstract: We experimentally characterize the non-equilibrium, room-temperature magnetization dynamics of a spin chain evolving under an effective double-quantum (DQ) Hamiltonian. We show that the Liouville space operators corresponding to the magnetization and the two-spin correlations evolve 90 degrees out of phase with each other, and drive the transport dynamics. For a nearest-neighbor-coupled N -spin chain, the dynamics are found to be restricted to a Liouville operator space whose dimension scales only as N 2 , leading to a slow growth of multi-spin correlations. Even though long-range couplings are present in the real system, we find excellent agreement between the analytical predictions and our experimental results, confirming that leakage out of the restricted Liouville space is slow on the timescales investigated. Our results indicate that the group velocity of the magnetization is6.04 ± 0.38 μ m s −1 , corresponding to a coherent transport over N ≈ 26 spins on the experimental timescale. As the DQ Hamiltonian is related to the standard one-dimensional XX Hamiltonian by a similarity transform, our results can be directly extended to XX quantum spin chains, which have been extensively studied in the context of both quantum magnetism and quantum information processing. | |
BibTeX:
@article{Ramanathan11, author = {Chandrasekhar Ramanathan and Paola Cappellaro and Lorenza Viola and David G Cory}, title = {Experimental characterization of coherent magnetization transport in a one-dimensional spin system}, journal = {New J. Phys.}, year = {2011}, volume = {13}, number = {10}, pages = {103015}, doi = {10.1088/1367-2630/13/10/103015} } |
|
2010 | UP ↑ |
Systems & Control Letters 59, 782 - 786 (2010) |
|
Abstract: In Nuclear Magnetic Resonance (NMR) spectroscopy, the measurement of the collective spin magnetization is weakly invasive and its back-action is called radiation damping. The aim of this paper is to provide a control-theoretical analysis of the problem of suppressing radiation damping effects. We show that the various real-time feedback schemes commonly used in NMR can be cast in terms of high gain feedback, of exact cancellation based on knowledge of the radiation damping field, and of 2-degree of freedom control designs, with the exact cancellation as prefeedback. We further show that the formulation in control-theoretical terms naturally leads to devising other possible closed-loop schemes, such as a general high gain feedback stabilization design not requiring the knowledge of the radiation damping field. | |
BibTeX:
@article{Altafini10, author = {C. Altafini and P. Cappellaro and D. Cory}, title = {Feedback schemes for radiation damping suppression in NMR: A control-theoretical perspective}, journal = {Systems & Control Letters}, year = {2010}, volume = {59}, number = {12}, pages = {782 - 786}, doi = {10.1016/j.sysconle.2010.09.004} } |
|
ArXiv:1001.4804 (2010) |
|
Abstract: We present a new proof of the quantum Cramer-Rao bound for precision parameter estimation [1-3] and extend it to a more general class of measurement procedures. We analyze a generalized framework for parameter estimation that covers most experimentally accessible situations, where multiple rounds of measurements, auxiliary systems or external control of the evolution are available. The proof presented demonstrates the equivalence of these more general metrology procedures to the simplest optimal strategy for which the bound is proven: a single measurement of a two-level system interacting with a time-independent Hamiltonian. | |
BibTeX:
@article{Goldstein10x, author = {Goldstein, G. and Lukin, M.~D. and Cappellaro, P.}, title = {Quantum Limits on Parameter Estimation}, journal = {ArXiv:1001.4804}, year = {2010} } |
|
J. Chem. Phys. 133, 124105 (2010) |
|
Abstract: Magnetic resonance imaging can characterize and discriminate among tissues using their diverse physical and biochemical properties. Unfortunately, submicrometer screening of biological specimens is presently not possible, mainly due to lack of detection sensitivity. Here we analyze the use of a nitrogen-vacancy center in diamond as a magnetic sensor for nanoscale nuclear spin imaging and spectroscopy. We examine the ability of such a sensor to probe the fluctuations of the "classical" dipolar field due to a large number of neighboring nuclear spins in a densely protonated sample. We identify detection protocols that appropriately take into account the quantum character of the sensor and find a signal-to-noise ratio compatible with realistic experimental parameters. Through various example calculations we illustrate different kinds of image contrast. In particular, we show how to exploit the comparatively long nuclear spin correlation times to reconstruct a local, high-resolution sample spectrum. | |
BibTeX:
@article{Meriles10, author = {Carlos A. Meriles and Liang Jiang and Garry Goldstein and Jonathan S. Hodges and Jeronimo Maze and Mikhail D. Lukin and Paola Cappellaro}, title = {Imaging mesoscopic nuclear spin noise with a diamond magnetometer}, journal = {J. Chem. Phys.}, publisher = {AIP}, year = {2010}, volume = {133}, number = {12}, pages = {124105}, doi = {10.1063/1.3483676} } |
|
Phys. Rev. B 82, 201201 (2010) |
|
Abstract: We present an experimental and theoretical study of electronic spin decoherence in ensembles of nitrogen-vacancy (NV) color centers in bulk high-purity diamond at room temperature. Under appropriate conditions, we find ensemble NV spin coherence times (T2) comparable to that of single NV with T2>600??s for a sample with natural abundance of 13C and paramagnetic impurity density ?1015?cm?3. We also observe a sharp decrease in the coherence time with misalignment of the static magnetic field relative to the NV electronic spin axis, consistent with theoretical modeling of NV coupling to a 13C nuclear-spin bath. The long coherence times and increased signal-to-noise provided by room-temperature NV ensembles will aid many applications of NV centers in precision magnetometry and quantum information. | |
BibTeX:
@article{Stanwix10, author = {Stanwix, P. L. and Pham, L. M. and Maze, J. R. and Le Sage, D. and Yeung, T. K. and Cappellaro, P. and Hemmer, P. R. and Yacoby, A. and Lukin, M. D. and Walsworth, R. L.}, title = {Coherence of nitrogen-vacancy electronic spin ensembles in diamond}, journal = {Phys. Rev. B}, year = {2010}, volume = {82}, pages = {201201}, doi = {10.1103/PhysRevB.82.201201} } |
|
2009 | UP ↑ |
In Decision and Control, 2009 held jointly with the 2009 28th Chinese Control Conference. CDC/CCC 2009. Proceedings of the 48th IEEE Conference on , 1445 -1450 (2009) |
|
Abstract: In NMR spectroscopy, the collective measurement is weakly invasive and its back-action is called radiation damping. The aim of this paper is to provide a control-theoretical analysis of the problem of suppressing this radiation damping. It is shown that the two feedback schemes commonly used in the NMR practice correspond one to a high gain output feedback for the simple case of maintaining the spin 1/2 in its inverted state, and the second to a 2-degree of freedom control design with a prefeedback that exactly cancels the radiation damping field. A general high gain feedback stabilization design not requiring the knowledge of the radiation damping time constant is also investigated. | |
BibTeX:
@inproceedings{Altafini09, author = {Altafini, C. and Cappellaro, P. and Cory, D.}, title = {Feedback schemes for radiation damping suppression in NMR: a control-theoretical perspective}, booktitle = {Decision and Control, 2009 held jointly with the 2009 28th Chinese Control Conference. CDC/CCC 2009. Proceedings of the 48th IEEE Conference on}, year = {2009}, pages = {1445 -1450}, doi = {10.1109/CDC.2009.5400761} } |
|
Phys. Rev. Lett. 102, 210502 (2009) |
|
Abstract: We consider a protocol for the control of few-qubit registers comprising one electronic spin embedded in a nuclear spin bath. We show how to isolate a few proximal nuclear spins from the rest of the bath and use them as building blocks for a potentially scalable quantum information processor. We describe how coherent control techniques based on magnetic resonance methods can be adapted to these solid-state spin systems, to provide not only efficient, high fidelity manipulation but also decoupling from the spin bath. As an example, we analyze feasible performances and practical limitations in the realistic setting of nitrogen-vacancy centers in diamond. | |
BibTeX:
@article{Cappellaro09, author = {P. Cappellaro and L. Jiang and J. S. Hodges and M. D. Lukin}, title = {Coherence and Control of Quantum Registers Based on Electronic Spin in a Nuclear Spin Bath}, journal = {Phys. Rev. Lett.}, year = {2009}, volume = {102}, number = {21}, pages = {210502}, doi = {10.1103/PhysRevLett.102.210502} } |
|
Phys. Rev. A 80, 032311 (2009) |
|
Abstract: We propose a strategy to generate a many-body entangled state in a collection of randomly placed, dipolarly coupled electronic spins in the solid state. By using coherent control to restrict the evolution into a suitable collective subspace, this method enables the preparation of GHZ-like and spin-squeezed states even for randomly positioned spins, while in addition protecting the entangled states against decoherence. We consider the application of this squeezing method to improve the sensitivity of nanoscale magnetometer based on nitrogen-vacancy spin qubits in diamond. | |
BibTeX:
@article{Cappellaro09b, author = {P. Cappellaro and M. D. Lukin}, title = {Quantum correlation in disordered spin systems: Applications to magnetic sensing}, journal = {Phys. Rev. A}, year = {2009}, volume = {80}, number = {3}, pages = {032311}, doi = {10.1103/PhysRevA.80.032311} } |
|
21st International Conference on Atomic Physics 21, 78 (2009) |
|
Abstract: The detection of weak magnetic fields with high spatial resolution is an outstanding problem in diverse areas ranging from fundamental physics and material science to data storage and bio-imaging. Here we describe an innovative approach to magnetometry that takes advantage of recently developed techniques for coherent control of solid-state spin qubits. We experimentally demonstrate this novel magnetometer employing an individual electronic spin associated with a Nitrogen-Vacancy (NV) center in diamond. Using an ultra-pure diamond sample, we achieve shot-noise-limited detection of nanotesla magnetic fields at kHz frequencies after 100 seconds of averaging. In addition, we demonstrate 0.5 microtesla/$Hz$ sensitivity for a diamond nanocrystal with volume of (30 nm)$^3$. This magnetic sensor provides an unprecedented combination of high sensitivity and spatial resolution --potentially allowing for the detection of a single nuclear spin's precession within one second. | |
BibTeX:
@inproceedings{Cappellaro09p, author = {Cappellaro, P. and Maze, JM and Childress, L. and Dutt, MVG and Hodges, JS and Hong, S. and Jiang, L. and Stanwix, PL and Taylor, JM and Togan, E. and others}, title = {Quantum Control of Spins and Photons at Nanoscales}, journal = {21st International Conference on Atomic Physics}, publisher = {World Scientific}, year = {2009}, volume = {21}, pages = {78}, doi = {10.1142/9789814273008_0009} } |
|
Advanced Optical Concepts in Quantum Computing, Memory, and Communication II In Advanced Optical Concepts in Quantum Computing, Memory, and Communication II 7225, 722509 (2009) |
|
Abstract: The ability to sense nanotelsa magnetic fields with nanoscale spatial resolution is an outstanding technical challenge relevant to the physical and biological sciences. For example, detection of such weak localized fields will enable sensing of magnetic resonance signals from individual electron or nuclear spins in complex biological molecules and the readout of classical or quantum bits of information encoded in an electron or nuclear spin memory. Here we present a novel approach to nanoscale magnetic sensing based on coherent control of an individual electronic spin contained in the Nitrogen-Vacancy (NV) center in diamond. At room temperature, using an ultra-pure diamond sample, we achieve shot-noise-limited detection of 3 nanotesla magnetic fields oscillating at kHz frequencies after 100 seconds of signal averaging. Furthermore, we experimentally demonstrate nanoscale resolution using a diamond nanocrystal of 30 nm diameter for which we achieve a sensitivity of 0.5 microtesla / Hz1/2. | |
BibTeX:
@inproceedings{Maze09p, author = {J. R. Maze and P. Cappellaro and L. Childress and M. V. G. Dutt and J. S. Hodges and S. Hong and L. Jiang and P. L. Stanwix and J. M. Taylor and E. Togan and A. S. Zibrov and P. Hemmer and A. Yacoby and R. L. Walsworth and M. D. Lukin}, editor = {Zameer U. Hasan and Alan E. Craig and Philip R. Hemmer}, title = {Nanoscale magnetic sensing using spin qubits in diamond}, booktitle = {Advanced Optical Concepts in Quantum Computing, Memory, and Communication II}, journal = {Advanced Optical Concepts in Quantum Computing, Memory, and Communication II}, publisher = {SPIE}, year = {2009}, volume = {7225}, number = {1}, pages = {722509}, doi = {10.1117/12.813802} } |
|
Phys. Rev. B 79, 041302 (2009) |
|
Abstract: We describe a technique that enables a strong coherent coupling between a single electronic spin qubit associated with a nitrogen-vacancy impurity in diamond and the quantized motion of a magnetized nanomechanical resonator tip. This coupling is achieved via careful preparation of dressed spin states which are highly sensitive to the motion of the resonator but insensitive to perturbations from the nuclear-spin bath. In combination with optical pumping techniques, the coherent exchange between spin and motional excitations enables ground-state cooling and controlled generation of arbitrary quantum superpositions of resonator states. Optical spin readout techniques provide a general measurement toolbox for the resonator with quantum limited precision. | |
BibTeX:
@article{Rabl09, author = {P. Rabl and P. Cappellaro and M. V. Gurudev Dutt and L. Jiang and J. R. Maze and M. D. Lukin}, title = {Strong magnetic coupling between an electronic spin qubit and a mechanical resonator}, journal = {Phys. Rev. B}, year = {2009}, volume = {79}, number = {4}, pages = {041302}, doi = {10.1103/PhysRevB.79.041302} } |
|
Phys. Rev. A 80, 052323 (2009) |
|
Abstract: The 19F spins in a crystal of fluorapatite have often been used to experimentally approximate a one-dimensional spin system. Under suitable multipulse control, the nuclear-spin dynamics may be modeled to first approximation by a double-quantum one-dimensional Hamiltonian, which is analytically solvable for nearest-neighbor couplings. Here, we use solid-state nuclear magnetic resonance techniques to investigate the multiple quantum coherence dynamics of fluorapatite, with an emphasis on understanding the region of validity for such a simplified picture. Using experimental, numerical, and analytical methods, we explore the effects of long-range intrachain couplings, cross-chain couplings, as well as couplings to a spin environment, all of which tend to damp the oscillations of the multiple quantum coherence signal at sufficiently long times. Our analysis characterizes the extent to which fluorapatite can faithfully simulate a one-dimensional quantum wire. | |
BibTeX:
@article{Zhang09, author = {Zhang, Wenxian and Cappellaro, Paola and Antler, Natania and Pepper, Brian and Cory, David G. and Dobrovitski, Viatcheslav V. and Ramanathan, Chandrasekhar and Viola, Lorenza}, title = {NMR multiple quantum coherences in quasi-one-dimensional spin systems: Comparison with ideal spin-chain dynamics}, journal = {Phys. Rev. A}, year = {2009}, volume = {80}, number = {5}, pages = {052323}, doi = {10.1103/PhysRevA.80.052323} } |
|
2008 | UP ↑ |
Phys. Rev. Lett. 100, 073001 (2008) |
|
Abstract: We investigate the coherence properties of individual nuclear spin quantum bits in diamond [Dutt et al., Science 316, 1312 (2007)] when a proximal electronic spin associated with a nitrogen-vacancy (N-V) center is being interrogated by optical radiation. The resulting nuclear spin dynamics are governed by time-dependent hyperfine interaction associated with rapid electronic transitions, which can be described by a spin-fluctuator model. We show that due to a process analogous to motional averaging in nuclear magnetic resonance, the nuclear spin coherence can be preserved after a large number of optical excitation cycles. Our theoretical analysis is in good agreement with experimental results. It indicates a novel approach that could potentially isolate the nuclear spin system completely from the electronic environment. | |
BibTeX:
@article{Jiang08, author = {L. Jiang and M. V. Gurudev Dutt and E. Togan and L. Childress and P. Cappellaro and J. M. Taylor and M. D. Lukin}, title = {Coherence of an Optically Illuminated Single Nuclear Spin Qubit}, journal = {Phys. Rev. Lett.}, year = {2008}, volume = {100}, number = {7}, pages = {073001}, doi = {10.1103/PhysRevLett.100.073001} } |
|
Nature 455, 644-647 (2008) |
|
Abstract: Detection of weak magnetic fields with nanoscale spatial resolution is an outstanding problem in the biological and physical sciences. For example, at a distance of 10 nm, the spin of a single electron produces a magnetic field of about 1 muT, and the corresponding field from a single proton is a few nanoteslas. A sensor able to detect such magnetic fields with nanometre spatial resolution would enable powerful applications, ranging from the detection of magnetic resonance signals from individual electron or nuclear spins in complex biological molecules to readout of classical or quantum bits of information encoded in an electron or nuclear spin memory. Here we experimentally demonstrate an approach to such nanoscale magnetic sensing, using coherent manipulation of an individual electronic spin qubit associated with a nitrogen-vacancy impurity in diamond at room temperature8. Using an ultra-pure diamond sample, we achieve detection of 3 nT magnetic fields at kilohertz frequencies after 100 s of averaging. In addition, we demonstrate a sensitivity of 0.5 muT Hz-1/2 for a diamond nanocrystal with a diameter of 30 nm. | |
BibTeX:
@article{Maze08, author = {J. R. Maze and P. L. Stanwix and J. S. Hodges and S. Hong and J. M. Taylor and P. Cappellaro and L. Jiang and A.S. Zibrov and A. Yacoby and R. Walsworth and M. D. Lukin}, title = {Nanoscale magnetic sensing with an individual electronic spin qubit in diamond}, journal = {Nature}, year = {2008}, volume = {455}, pages = {644--647}, doi = {10.1038/nature07279} } |
|
Nat Phys. 4, 810-816 (2008) |
|
Abstract: The detection of weak magnetic fields with high spatial resolution is an important problem in diverse areas ranging from fundamental physics and material science to data storage and biomedical science. Here, we explore a novel approach to the detection of weak magnetic fields that takes advantage of recently developed techniques for the coherent control of solid-state electron spin quantum bits. Specifically, we investigate a magnetic sensor based on nitrogen-vacancy centres in room-temperature diamond. We discuss two important applications of this technique: a nanoscale magnetometer that could potentially detect precession of single nuclear spins and an optical magnetic-field imager combining spatial resolution ranging from micrometres to millimetres with a sensitivity approaching a few fT Hz-1/2. | |
BibTeX:
@article{Taylor08, author = {Taylor, J. M. and Cappellaro, P. and Childress, L. and Jiang, L. and Budker, D. and Hemmer, P. R. and Yacoby, A. and Walsworth, R. and Lukin, M. D.}, title = {High-sensitivity diamond magnetometer with nanoscale resolution}, journal = {Nat Phys.}, publisher = {Nature Publishing Group}, year = {2008}, volume = {4}, number = {10}, pages = {810--816}, doi = {10.1038/nphys1075} } |
|
2007 | UP ↑ |
Phys. Rev. A 75, 042321 (2007) |
|
Abstract: A critical step in experimental quantum information processing (QIP) is to implement control of quantum systems protected against decoherence via informational encodings, such as quantum error-correcting codes, noiseless subsystems, and decoherence-free subspaces. These encodings lead to the promise of fault-tolerant QIP, but they come at the expense of resource overheads. Part of the challenge in studying control over multiple logical qubits is that QIP testbeds have not had sufficient resources to analyze encodings beyond the simplest ones. The most relevant resources are the number of available qubits and the cost to initialize and control them. Here we demonstrate an encoding of logical information that permits control over multiple logical qubits without full initialization, an issue that is particularly challenging in liquid-state NMR. The method of subsystem pseudopure states will allow the study of decoherence control schemes on up to six logical qubits using liquid-state NMR implementations. | |
BibTeX:
@article{Cappellaro07, author = {Cappellaro, P. and Hodges, J. S. and Havel, T. F. and Cory, D. G.}, title = {Subsystem pseudopure states}, journal = {Phys. Rev. A}, year = {2007}, volume = {75}, pages = {042321}, doi = {10.1103/PhysRevA.75.042321} } |
|
Phys. Rev. A 76, 032317 (2007) |
|
Abstract: We study experimentally a system comprised of linear chains of spin-1/2 nuclei that provides a test bed for multibody dynamics and quantum-information processing. This system is a paradigm for a class of quantum-information processing devices that can perform particular tasks even without universal control of the whole quantum system. We investigate the extent of control achievable on the system with current experimental apparatus and methods to gain information on the system state, when full tomography is not possible and in any case highly inefficient. | |
BibTeX:
@article{Cappellaro07a, author = {P. Cappellaro and C. Ramanathan and D. G. Cory}, title = {Dynamics and control of a quasi-one-dimensional spin system}, journal = {Phys. Rev. A}, year = {2007}, volume = {76}, number = {3}, pages = {032317}, doi = {10.1103/PhysRevA.76.032317} } |
|
Phys. Rev. Lett. 99, 250506 (2007) |
|
Abstract: Transport of quantum information in linear spin chains has been the subject of much theoretical work. Experimental studies by NMR in solid state spin systems (a natural implementation of such models) is complicated since the dipolar Hamiltonian is not solely comprised of nearest-neighbor XY-Heisenberg couplings. We present here a similarity transformation between the XY Hamiltonian and the double-quantum Hamiltonian, an interaction which is achievable with the collective control provided by radio-frequency pulses. Not only can this second Hamiltonian simulate the information transport in a spin chain, but it also creates coherent states, whose intensities give an experimental signature of the transport. This scheme makes it possible to study experimentally the transport of polarization beyond exactly solvable models and explore the appearance of quantum coherence and interference effects. | |
BibTeX:
@article{Cappellaro07l, author = {P. Cappellaro and C. Ramanathan and D. G. Cory}, title = {Simulations of Information Transport in Spin Chains}, journal = {Phys. Rev. Lett.}, year = {2007}, volume = {99}, number = {25}, pages = {250506}, doi = {10.1103/PhysRevLett.99.250506} } |
|
Las. Phys. 17, 545-551 (2007) |
|
Abstract: Decoherence-free subspaces protect quantum information from the effects of noise that is correlated across the physical qubits used to implement them. Given the ability to impose suitable Hamiltonians upon such a multi-qubit system, one can also implement a set of logical gates which enables universal computation on this information without compromising this protection. Real physical systems, however, seldom come with the correct Hamiltonians built-in, let alone the ability to turn them off and on at will. In the course of our development of quantum information processing devices based on liquid-state NMR, we have found the task of operating on quantum information encoded in decoherence-free subspaces rather more challenging than is commonly assumed. This contribution presents an overview of these challenges and the methods we have developed for overcoming them in practice. These methods promise to be broadly applicable to many of the physical systems proposed for the implementation of quantum information processing devices. | |
BibTeX:
@article{Cappellaro07p, author = {Cappellaro, P. and Hodges, J.~S. and Havel, T.~F. and Cory, D.~G.}, title = {Control of qubits encoded in decoherence-free subspaces}, journal = {Las. Phys.}, year = {2007}, volume = {17}, pages = {545-551}, doi = {10.1134/S1054660X0704038X} } |
|
Phys. Rev. A 75, 042320 (2007) |
|
Abstract: Liquid-phase NMR is a general-purpose testbed for developing methods of coherent control relevant to quantum information processing. Here we extend these studies to the coherent control of logical qubits and in particular to the unitary gates necessary to create entanglement between logical qubits. We report an experimental implementation of a conditional logical gate between two logical qubits that are each in decoherence-free subspaces that protect the quantum information from fully correlated dephasing. | |
BibTeX:
@article{Hodges07, author = {Hodges, J. S. and Cappellaro, P. and Havel, T. F. and Martinez, R. and Cory, D. G.}, title = {Experimental implementation of a logical Bell state encoding}, journal = {Phys. Rev. A}, year = {2007}, volume = {75}, number = {4}, pages = {042320}, doi = {10.1103/PhysRevA.75.042320} } |
|
2006 | UP ↑ |
J. Chem. Phys. 125, 044514 (2006) |
|
Abstract: Decoherence-free subsystems (DFSs) are a powerful means of protecting quantum information against noise with known symmetry properties. Although Hamiltonians that can implement a universal set of logic gates on DFS encoded qubits without ever leaving the protected subsystem theoretically exist, the natural Hamiltonians that are available in specific implementations do not necessarily have this property. Here we describe some of the principles that can be used in such cases to operate on encoded qubits without losing the protection offered by the DFSs. In particular, we show how dynamical decoupling can be used to control decoherence during the unavoidable excursions outside of the DFS. By means of cumulant expansions, we show how the fidelity of quantum gates implemented by this method on a simple two physical qubit DFS depends on the correlation time of the noise responsible for decoherence. We further show by means of numerical simulations how our previously introduced ?strongly modulating pulses? for NMR quantum information processing can permit high-fidelity operations on multiple DFS encoded qubits in practice, provided that the rate at which the system can be modulated is fast compared to the correlation time of the noise. The principles thereby illustrated are expected to be broadly applicable to many implementations of quantum information processors based on DFS encoded qubits. | |
BibTeX:
@article{Cappellaro06, author = {Cappellaro, P. and Hodges, J. S. and Havel, T. F. and Cory, D. G}, title = {Principles of Control for Decoherence-Free Subsystems}, journal = {J. Chem. Phys.}, year = {2006}, volume = {125}, pages = {044514}, doi = {10.1063/1.2216702} } |
|
In Quantum Computing in Solid State Systems , 306-312 (2006) |
|
Abstract: A new approach to the measurement of the state of a collapsed single spin is described by using many entangled spins as an amplifier. A single target spin is coupled via the natural dipolar Hamiltonian to a large collection of spins. Applying external radio frequency (r.f.) pulses, we can control the evolution of the system so that the ensemble spins reach one of two orthogonal states whose collective properties differ depending on the state of the target spin and are easily measured. The result of an experiment simulating this method on an ensemble liquid state NMR quantum processor is reported. That entanglement assisted metrology is compatible with the real control we have over physical spins is suggested, since the measurement process can actually be described in terms of the physical Hamiltonian of the spin system. By building on this work, and with the needed technical advances, it should be possible to detect a single nuclear spin. | |
BibTeX:
@incollection{Cappellaro06p, author = {Cappellaro, Paola and Emerson, Joseph and Boulant, Nicolas and Ramanathan, Chandrasekhar and Lloyd, Seth and Cory, David G.}, editor = {Ruggiero, B. and Delsing, P. and Granata, C. and Pashkin, Y. and Silvestrini, P.}, title = {Spin amplifier for single spin measurement}, booktitle = {Quantum Computing in Solid State Systems}, publisher = {Springer New York}, year = {2006}, pages = {306-312}, doi = {10.1007/0-387-31143-2_37} } |
|
Thesis at: Massachusetts Institute of Technology, Department of Nuclear Science and Engineering (2006) |
|
Abstract: Coherence and entanglement in multi-spin systems are valuable resources for quantum information processing. In this thesis, I explore the manipulation of quantum information in complex multi-spin systems, with particular reference to Nuclear Magnetic Resonance implementations. In systems with a few spins, such as molecules in the liquid phase, the use of multi-spin coherent states provides a hedge against the noise, via the encoding of information in logical degrees of freedom distributed over several spins. Manipulating multi-spin coherent states also increases the complexity of quantum operations required in a quantum processor. Here I present schemes to mitigate this problem, both in the state initialization, with particular attention to bulk ensemble quantum information processing, and in the coherent control and gate implementations. In the many-body limit provided by nuclear spins in single crystals, the limitations in the available control increase the complexity of manipulating the system; also, the equations of motion are no longer exactly solvable even in the closed-system limit. Entanglement and multi-spin coherences are essential for extending the control and the accessible information on the system. I employ entanglement in a large ensemble of spins in order to obtain an amplification of the small perturbation created by a single spin on the spin ensemble, in a scheme for the measurement of a single nuclear spin state. I furthermore use multiple quantum coherences in mixed multi-spin states as a tool to explore many-body behavior of linear chain of spins, showing their ability to perform quantum information processing tasks such as simulations and transport of information. The theoretical and experimental results of this thesis suggest that although coherent multi-spin states are particularly fragile and complex to control they could make possible the execution of quantum information processing tasks that have no classical counterparts. | |
BibTeX:
@phdthesis{Cappellaro06t, author = {Paola Cappellaro}, title = {Quantum Information Processing in Multi-Spin Systems}, school = {Massachusetts Institute of Technology}, year = {2006} } |
|
Phys. Rev. B 74, 224434 (2006) |
|
Abstract: We have measured the decay of NMR multiple quantum coherence intensities both under the internal dipolar Hamiltonian as well as when this interaction is effectively averaged to zero, in the cubic calcium fluoride (CaF2) spin system and the pseudo-one-dimensional system of fluoroapatite. In calcium fluoride the decay rates depend both on the number of correlated spins in the cluster, as well as on the coherence number. For smaller clusters, the decays depend strongly on coherence number, but this dependence weakens as the size of the cluster increases. The same scaling was observed when the coherence distribution was measured in both the usual Zeeman or z basis and the x basis. The coherence decay in the one-dimensional fluoroapatite system did not change significantly as a function of the multiple quantum growth time, in contrast to the calcium fluoride case. While the growth of coherence orders is severely restricted in this case, the number of correlated spins should continue to grow, albeit more slowly. All coherence intensities were observed to decay as Gaussian functions in time. In all cases the standard deviation of the observed decay appeared to scale linearly with coherence number. | |
BibTeX:
@article{Cho06, author = {Hyung Joon Cho and Paola Cappellaro and David G. Cory and Chandrasekhar Ramanathan}, title = {Decay of highly correlated spin states in a dipolar-coupled solid: NMR study of CaF2}, journal = {Phys. Rev. B}, year = {2006}, volume = {74}, number = {22}, pages = {224434}, doi = {10.1103/PhysRevB.74.224434} } |
|
In Decision and Control, 2006 45th IEEE Conference on , 2488 -2494 (2006) |
|
Abstract: Nuclear magnetic resonance (NMR) spectroscopy has proven to be a facile means of achieving small-scale demonstrations of quantum information processing. This was in large part made possible by the sophisticated methods of quantum control that have been developed by the NMR community over a span of more than 50 years. The traditional control methods, already perhaps the most complex examples of open-loop control available, were nevertheless designed primarily to assist in identifying the physical parameters of the underlying spin system, rather than to control the system with high precision. We have therefore extended the traditional methods in a variety of ways so as to achieve precise control, by taking advantage of prior knowledge of the physical parameters as determined by traditional methods. Due to the experimental challenges of real-time control, these developments relied upon our ability to simulate the evolution of the system under the action of radio-frequency control fields with essentially arbitrary precision, subject only to the available computing power. This talk presents an overview of our work in quantum control together with some of the on-going challenges still facing us | |
BibTeX:
@inproceedings{Hodges06, author = {Hodges, J. and Cappellaro, P. and Havel, T.F. and Cory, D.G.}, title = {Quantum Control of Nuclear Spins}, booktitle = {Decision and Control, 2006 45th IEEE Conference on}, year = {2006}, pages = {2488 -2494}, doi = {10.1109/CDC.2006.377562} } |
|
Phys. Rev. Lett. 97, 100501 (2006) |
|
Abstract: We analyze a conceptual approach to single-spin measurement. The method uses techniques from the theory of quantum cellular automata to correlate a large number of ancillary spins to the one to be measured. It has the distinct advantage of being efficient: under ideal conditions, it requires the application of only O(3 N) steps (each requiring a constant number of rf pulses) to create a system of N correlated spins. Numerical simulations suggest that it is also, to a certain extent, robust against pulse errors, and imperfect initial polarization of the ancilla spin system. | |
BibTeX:
@article{Perez-Delgado06, author = {Carlos A. Perez-Delgado and Michele Mosca and Paola Cappellaro and David G. Cory}, title = {Single Spin Measurement Using Cellular Automata Techniques}, journal = {Phys. Rev. Lett.}, year = {2006}, volume = {97}, number = {10}, pages = {100501}, doi = {10.1103/PhysRevLett.97.100501} } |
|
2005 & Earlier | UP ↑ |
Phys. Rev. Lett. 94, 020502 (2005) |
|
Abstract: We propose a new approach to the measurement of a single spin state, based on nuclear magnetic resonance (NMR) techniques and inspired by the coherent control over many-body systems envisaged by quantum information processing. A single target spin is coupled via the magnetic dipolar interaction to a large ensemble of spins. Applying radio frequency pulses, we can control the evolution so that the spin ensemble reaches one of two orthogonal states whose collective properties differ depending on the state of the target spin and are easily measured. We first describe this measurement process using quantum gates; then we show how equivalent schemes can be defined in terms of the Hamiltonian and thus implemented under conditions of real control, using well established NMR techniques. We demonstrate this method with a proof of principle experiment in ensemble liquid state NMR and simulations for small spin systems. | |
BibTeX:
@article{Cappellaro05, author = {Paola Cappellaro and Joseph Emerson and Nicolas Boulant and Chandrasekhar Ramanathan and Seth Lloyd and David G Cory}, title = {Entanglement Assisted Metrology}, journal = {Phys. Rev. Lett.}, year = {2005}, volume = {94}, pages = {020502}, doi = {10.1103/PhysRevLett.94.020502} } |
|
In Technical Proceedings of the 2005 NSTI Nanotechnology Conference and Trade Show 3, 161 - 164 (2005) |
|
Abstract: This talk will illustrate the benefits offered by QIP with two devices which use quantum entanglement among nuclear spins to defeat the Heisenberg limits: (1) a spin gyroscope that operates by detecting the frequency shift in the spins? precession rate in the rotating frame, which is potentially more accurate than mechanical or optical devices; (2) a quantum amplifier which correlates the states of a macroscopic number of nuclear spins with the state of a single target spin, so that a collective measurement of the state of the amplifier?s spins reveals that of the target spin. | |
BibTeX:
@inproceedings{Havel05, author = {T.F. Havel and P. Cappellaro and C. Ramanathan and D.G. Cory}, title = {Quantum Information Processing with Nuclear Spin-Based Devices}, booktitle = {Technical Proceedings of the 2005 NSTI Nanotechnology Conference and Trade Show}, year = {2005}, volume = {3}, pages = {161 - 164} } |
|
J. Mag. Res. 161, 132-137 (2003) |
|
Abstract: We present improved line-narrowing sequences for dipolar coupled spin systems, based on a train of magic-echoes which are compensated for the effects of finite pulse widths and utilize symmetry properties of supercycles. Sequences are introduced for spectroscopy and imaging by proper choice of a phase alternating scheme. Using a 16 pulse time-suspension magic-echo cycle, the highest level of line-narrowing achieved was 2.7 Hz for the [100] direction of a single crystal of calcium fluoride, a reduction in linewidth by 4 orders of magnitude. | |
BibTeX:
@article{Boutis03, author = {Boutis, G. S. and Cappellaro, P. and Cho, H. and Ramanathan, C. and Cory, D. G.}, title = {Pulse error compensating symmetric magic-echo trains}, journal = {J. Mag. Res.}, year = {2003}, volume = {161}, pages = {132-137}, doi = {10.1016/S1090-7807(03)00010-7} } |
|
Chem. Phys. Lett. 369, 311 (2003) |
|
Abstract: Multiple quantum (MQ) coherences are characterized by their coherence number and the number of spins that make up the state, though only the coherence number is normally measured. We present a simple set of measurements that extend our knowledge of the MQ state by recording the coherences in two non-commuting bases, the x and the z bases (related by a similarity transformation). The measurement of coherences in a basis other than the usual z basis also permits the study of spin dynamics under Hamiltonians that conserve z basis coherence number. | |
BibTeX:
@article{Ramanathan03, author = {Chandrasekhar Ramanathan and Hyungjoon Cho and Paola Cappellaro and Gregory S Boutis and David G Cory}, title = {Encoding multiple quantum coherences in non-commuting bases}, journal = {Chem. Phys. Lett.}, year = {2003}, volume = {369}, pages = {311}, doi = {10.1016/S0009-2614(02)02020-1} } |
|
In Proceedings of the 6th International Conference on Quantum Communication, Measurement and Computing. , 267-270 (2003) |
|
Abstract:Exploring large nuclear spin systems in the solid state using NMR. | |
BibTeX:
@inproceedings{Ramanathan03p, author = {C. Ramanathan, H. Cho, P.Cappellaro,G.S. Boutis and D.G. Cory}, editor = {Jeffrey H. Shapiro and Osamu Hirota}, title = {Exploring large nuclear spin systems in the solid state using NMR}, booktitle = {Proceedings of the 6th International Conference on Quantum Communication, Measurement and Computing.}, publisher = {Rinton Press}, year = {2003}, pages = {267-270} } |
|
In Advanced Monte Carlo for Radiation Physics, Particle Transport Simulation and Applications Berlin, Heidelberg , 1157-1162 (2001) |
|
Abstract: To improve the response to high-energy neutrons of a conventional Bonner Sphere Spectrometer, the response functions of several detector configurations of different sizes and materials were calculated with the Monte Carlo programme FLUKA. The two most promising configurations were selected, built and afterwards exposed to neutrons of an Am-Be source and to a broad high-energy neutron spectrum at CERN. The comparison between the measured and calculated detector responses of the new spheres in these radiation fields confirms their simulated response functions and justifies their implementation into the conventional Bonner Sphere Spectrometer. | |
BibTeX:
@inproceedings{Birattari01, author = {Birattari, C. and Cappellaro, P. and Mitaroff, A. and Silari, M.}, editor = {Kling, Andreas and Baro, Fernando J. C. and Nakagawa, Masayuki and Tavora, Luis and Vaz, Pedro}, title = {Development of an Extended Range Bonner Sphere Spectrometer}, booktitle = {Advanced Monte Carlo for Radiation Physics, Particle Transport Simulation and Applications}, publisher = {Springer Berlin Heidelberg}, year = {2001}, pages = {1157--1162} } |