Power sensitivity of NV-based RF detectors scales inversely with the physical size of the RF-spin interface, reaching estimated limits of 10^{-20} W Hz^{-1} (slope) and 10^{-12} W Hz^{-1/2} (variance) under photon shot noise.
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Sub-resonant charge cycling of NV centers arises from phonon-assisted anti-Stokes excitation, with low-energy acoustic phonons near the ZPL and a 43 meV mode at longer wavelengths contributing most.
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Power sensitivity of broadband radiofrequency detectors based on quantum diamond spins
Power sensitivity of NV-based RF detectors scales inversely with the physical size of the RF-spin interface, reaching estimated limits of 10^{-20} W Hz^{-1} (slope) and 10^{-12} W Hz^{-1/2} (variance) under photon shot noise.
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Phonon-assisted charge-cycling of nitrogen-vacancy centres in diamond
Sub-resonant charge cycling of NV centers arises from phonon-assisted anti-Stokes excitation, with low-energy acoustic phonons near the ZPL and a 43 meV mode at longer wavelengths contributing most.