Quantum sensing limits#
Quantum limits of a phase measurement, and the acceleration sensitivity of an atom interferometer.
A sensor that reads a phase \(\varphi\) from \(N\) independent probes (atoms, photons) repeated \(\nu\) times cannot do better than the standard quantum limit,
while entangled probes can in principle reach the Heisenberg limit \(\Delta\varphi_{\mathrm{H}} = 1/(N\sqrt{\nu})\). Entangled states are fragile, so real instruments sit near the standard quantum limit.
A light-pulse atom interferometer measures a constant acceleration \(a\) as a phase \(\varphi = k_{\mathrm{eff}}\, a\, T^2\), with \(k_{\mathrm{eff}} = 4\pi/\lambda\) the effective two-photon wave number and \(T\) the time between pulses (Kasevich and Chu, 1992). Its single-shot acceleration sensitivity is therefore \(\Delta a = \Delta\varphi/(C\, k_{\mathrm{eff}} T^2)\) with \(C\) the fringe contrast.
Functions
Smallest phase resolvable with |
|
Single-shot acceleration sensitivity of a light-pulse atom interferometer. |
Data
Wavelength of the rubidium-87 D2 line, a common choice for atom interferometers, in metres. |
- phase_sensitivity(n_probes, repeats=1, scaling='sql')[source]#
Smallest phase resolvable with
n_probesprobes repeatedrepeatstimes.- Parameters:
- Returns:
float– Phase uncertainty in radians.- Raises:
ValueError – For fewer than one probe or one repeat, or an unknown scaling.
Examples
>>> from quantum_mind.sensing import phase_sensitivity >>> round(phase_sensitivity(10_000), 4), round(phase_sensitivity(10_000, scaling='heisenberg'), 6) (0.01, 0.0001)
- atom_interferometer_sensitivity(n_atoms, interrogation_time, contrast=0.5, wavelength=7.8024e-07, scaling='sql')[source]#
Single-shot acceleration sensitivity of a light-pulse atom interferometer.
- Parameters:
- Returns:
float– Acceleration uncertainty per shot in m/s^2.
Examples
>>> from quantum_mind.sensing import atom_interferometer_sensitivity >>> a = atom_interferometer_sensitivity(1e6, 0.1) >>> 1e-9 < a < 1e-7 True
- RB87_WAVELENGTH_M#
Wavelength of the rubidium-87 D2 line, a common choice for atom interferometers, in metres.