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Magnetic-field-insensitive coherent-population-trapping resonances excited by bichromatic linearly polarized fields on the \\(D_1\\) line of \\(^{133}\\)Cs
by
Matsumoto, K
, Kagami, S
, Kirihara, A
, Morinaga, A
, Yanagimachi, S
, Ikegami, T
in
Atomic clocks
/ Excitation spectra
/ Frequency shift
/ Linear polarization
/ Magnetic fields
/ Magnetic resonance
/ Resonance
/ Trapping
2021
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Magnetic-field-insensitive coherent-population-trapping resonances excited by bichromatic linearly polarized fields on the \\(D_1\\) line of \\(^{133}\\)Cs
by
Matsumoto, K
, Kagami, S
, Kirihara, A
, Morinaga, A
, Yanagimachi, S
, Ikegami, T
in
Atomic clocks
/ Excitation spectra
/ Frequency shift
/ Linear polarization
/ Magnetic fields
/ Magnetic resonance
/ Resonance
/ Trapping
2021
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While trying to remove the title from your shelf something went wrong :( Kindly try again later!
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Magnetic-field-insensitive coherent-population-trapping resonances excited by bichromatic linearly polarized fields on the \\(D_1\\) line of \\(^{133}\\)Cs
by
Matsumoto, K
, Kagami, S
, Kirihara, A
, Morinaga, A
, Yanagimachi, S
, Ikegami, T
in
Atomic clocks
/ Excitation spectra
/ Frequency shift
/ Linear polarization
/ Magnetic fields
/ Magnetic resonance
/ Resonance
/ Trapping
2021
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Magnetic-field-insensitive coherent-population-trapping resonances excited by bichromatic linearly polarized fields on the \\(D_1\\) line of \\(^{133}\\)Cs
Paper
Magnetic-field-insensitive coherent-population-trapping resonances excited by bichromatic linearly polarized fields on the \\(D_1\\) line of \\(^{133}\\)Cs
2021
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Overview
We have experimentally demonstrated that magnetic-field-insensitive coherent-population-trapping (CPT) resonances are generated between the ground hyperfine levels on the \\(D_1\\) line of \\(^{133}\\)Cs using a two-photon \\(\\Lambda\\) scheme excited by lin || lin polarizations. The frequency shift of the CPT resonance is 0.04 Hz for the deviation of 1 \\(\\mu\\)T at a \"magic\" magnetic field of 139 \\(\\mu\\)T and is 50 times smaller than that of the conventional clock transition at a typical bias magnetic field for the clock operation. The amplitude of the CPT spectrum excited by lin || lin polarizations is enhanced as the excitation intensity increases and is well explained by the three-level model without trap levels. Thus, the CPT resonance on the \\(D_1\\) line of \\(^{133}\\)Cs atom excited by a simple lin || lin scheme will be one of the best candidates for frequency reference of miniature atomic clocks.
Publisher
Cornell University Library, arXiv.org
Subject
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