Atom interferometry using σ+σ^+-σ−σ^- Raman transitions between F=1,mF=∓1F=1,m_F=\mp1 and F=2,mF=±1F=2,m_F=\pm1

preprint2021arXivOpen access

Abstract

We report on the experimental demonstration of a horizontal accelerometer based on atom interferometry using counterpropagative Raman transitions between the states F=1,mF=∓1F=1,m_F=\mp1 and F=2,mF=±1F=2,m_F=\pm1 of 87^{87}Rb. Compared to the F=1,mF=0↔F=2,mF=0F=1,m_F=0 \leftrightarrow F=2,m_F=0 transition usually used in atom interferometry, our scheme presents the advantages to have only a single counterpropagating transition allowed in a retroreected geometry, to use the same polarization configuration than the magneto-optical trap and to allow the control of the atom trajectory with magnetic forces. We demonstrate horizontal acceleration measurement in a close-to-zero velocity regime using a singlediffraction Raman process with a short-term sensitivity of 25×10−525 \times 10^{-5} m.s−2^{-2}.Hz−1/2^{-1/2}. We discuss specific features of the technique such as spontaneous emission, light-shifts and effects of magnetic field inhomogeneities. We finally give possible applications of this technique in metrology or for cold-atom inertial sensors dedicated to onboard applications.

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