Conceitos Básicos
Microwave phase noise is a significant limiting factor in the sensitivity of NV center diamond magnetometers, especially at high carrier frequencies and for long measurement times, but mitigation strategies like gradiometry and optimized pulse sequences can suppress its impact.
Estatísticas
The noise floor off resonance is ηoff ≈6.0 pTrms s1/2, consistent with the expected noise floor in the photoelectron-shot-noise limit, ηpsn ≈5.4 pTrms s1/2.
Measurements with G2 detuned by +0.4 GHz from f+ have the same noise floor.
The non-zero values, {ηex,−≈4.7 pTrms s1/2, ηex,+≈11.9 pTrms s1/2}, indicate additional noise that is only present when G2 is tuned to resonance.
For a 1-kHz bandwidth magnetometer, the phase-noise-limited equivalent magnetic sensitivity is ∼1.4 pTrms s1/2 for G1 operated at fG1 = 2.5 GHz and ∼0.3 pTrms s1/2 for G2 operated at fG2 = 2.1 GHz.
The gradiometer noise floor exhibits a 14 pTrms s1/2/√t scaling for the duration of the measurement, dropping below 200 fTrms for t = 5000 s.
The gradient signal peak remains at 14.7 ± 0.5 nTrms over the course of the measurement.
Citações
"MW phase noise from typical MW generators produces NV sensor noise at the level of 0.1-100 pTs1/2, orders of magnitude above requirements for applications like magnetoencephalography."
"Here we study the impact of microwave (MW) phase noise on the response of an NV sensor. Fluctuations of the phase of the MW waveform cause undesired rotations of the NV spin state. These fluctuations are imprinted in the optical readout signal and, left unmitigated, are indistinguishable from magnetic field noise."
"Our study highlights an important challenge in the pursuit of sensitive diamond quantum sensors and is applicable to other qubit systems with a large transition frequency."