Magnetometric sensitivity optimization for nonlinear optical rotation with frequency-modulated light: rubidium D2 line

TL;DR

This paper investigates how to optimize the sensitivity of nonlinear magneto-optical rotation measurements in rubidium atoms using frequency-modulated light, achieving extremely high precision in detecting magnetic fields and atomic energy shifts.

Contribution

It provides a detailed analysis of the factors affecting magnetometric sensitivity in rubidium D2 line using FM NMOR, and reports the optimal sensitivity achieved under specific conditions.

Findings

Optimal shot-noise-projected sensitivity of 2 x 10^{-11} G/Hz^{1/2}

Sensitivity to spin precession frequency of ~10 microHz/Hz^{1/2}

Sensitivity to Zeeman shifts of ~4 x 10^{-20} eV/Hz^{1/2}

Abstract

Atomic spin polarization of alkali atoms in the ground state can survive thousands of collisions with paraffin-coated cell walls. The resulting long spin-relaxation times achieved in evacuated, paraffin-coated cells enable precise measurement of atomic spin precession and energy shifts of ground-state Zeeman sublevels. In the present work, nonlinear magneto-optical rotation with frequency-modulated light (FM NMOR) is used to measure magnetic-field-induced spin precession for rubidium atoms contained in a paraffin-coated cell. The magnetometric sensitivity of FM NMOR for the rubidium D2 line is studied as a function of light power, detuning, frequency-modulation amplitude, and rubidium vapor density. For a 5-cm diameter cell at temperature T ~ 35 degrees C, the optimal shot-noise-projected magnetometric sensitivity is found to be 2 x 10^{-11} G/Hz^{1/2} (corresponding to a sensitivity to spin precession frequency of ~ 10 microHz/Hz^{1/2} or a sensitivity to Zeeman sublevel shifts of ~ 4 x 10^{-20} eV/Hz^{1/2}).