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Signal reception of nuclear magnetic resonance (NMR) usually relies on electrical amplification of the electromotive force caused by nuclear induction.
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2010
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A. A. Clerk, M. H. Devoret, S. M. Girvin, F. Marquardt, and R. J. Schoelkopf, Introduction to quantum noise, measurement, and amplification, Rev. Mod. Phys. 82
2010
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2010
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2010
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2011
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J. M. Taylor, A. S. Sørensen, C. M. Marcus, and E. S. Polzik, Laser Cooling and Optical Detection of Excitations in a LC Electrical Circuit, Phys. Rev. Lett. 107
2011
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2011
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M. C. Butler and D. P. Weitekamp, Polarization of nuclear spins by a cold nanoscale resonator, Phys. Rev. A 84
2011
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2014
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C. P. Slichter, The discovery and renaissance of dynamic nuclear polarization, Rep. Prog. Phys. 77
2014
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C. J. Wood, T. W. Borneman, and D. G. Cory, Cavity Cooling of an Ensemble Spin System, Phys. Rev. Lett. 112
2014
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2015
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C. J. Wood and D. G. Cory, Cavity Cooling to the Ground State of an Ensemble Quantum System, Phys. Rev. A 93
2016
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A. Bienfait, J. J. Pla, Y. Kubo, X. Zhou, M. Stern, C. C. Lo, C. D. Weis, T. Schenkel, D. Vion, D. Esteve, J. J. L. Morton, and P. Bertet, Controlling spin relaxation with a cavity, Nature 531
2016
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R. Hisatomi, A. Osada, Y. Tabuchi, T. Ishikawa, A. Noguchi, R. Yamazaki, K. Usami, and Y. Nakamura, Bidirectional conversion between microwave and light via ferromagnetic magnons, Phys. Rev. B 93
2016
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C. Eichler, A. J. Sigillito, S. A. Lyon, and J. R. Petta, Electron Spin Resonance at the Level of 10 4 Spins Using Low Impedance Superconducting Resonators, Phys. Rev. Lett. 118
2017
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