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Features of the Formation of the Spin Polarization of an Alkali Metal at the Resolution of Hyperfine Sublevels in the 2 S 1/2 State

The optical orientation of the angular momenta of alkali atoms in the presence of a buffer gas (molecular nitrogen) has been studied experimentally. It has been shown that, even at a low concentration of molecular nitrogen in the cell, the excitation of 133Cs atoms from the lower hyperfine level wit...

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Published in:JETP letters 2018-01, Vol.108 (8), p.513
Main Authors: Popov, E N, Bobrikova, V A, Voskoboinikov, S P, Barantsev, K A, Ustinov, S M, Litvinov, A N, Vershovskii, A K, Dmitriev, S P, Kartoshkin, V A, Pazgalev, A S, Petrenko, M V
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container_start_page 513
container_title JETP letters
container_volume 108
creator Popov, E N
Bobrikova, V A
Voskoboinikov, S P
Barantsev, K A
Ustinov, S M
Litvinov, A N
Vershovskii, A K
Dmitriev, S P
Kartoshkin, V A
Pazgalev, A S
Petrenko, M V
description The optical orientation of the angular momenta of alkali atoms in the presence of a buffer gas (molecular nitrogen) has been studied experimentally. It has been shown that, even at a low concentration of molecular nitrogen in the cell, the excitation of 133Cs atoms from the lower hyperfine level with F = 3, which belongs to the ground 2S1/2 state, results in a larger amplitude of the magnetic resonance than the excitation from the hyperfine level with F = 4. This result has been theoretically explained under the assumption that the spin state of the alkali atomic nucleus does not change at collision with a nitrogen molecule, which is accompanied by a nonradiative transition of the alkali atom from the excited 2P1/2 state to the ground 2S1/2 state.
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subjects Alkali metals
Cesium 133
Cesium isotopes
Excitation
Magnetic resonance
Nitrogen
Nuclei (nuclear physics)
Polarization (spin alignment)
title Features of the Formation of the Spin Polarization of an Alkali Metal at the Resolution of Hyperfine Sublevels in the 2 S 1/2 State
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