Secondary laser cooling and capturing of thulium atoms in traps

Secondary laser cooling has been realised on the weak dipole transition , , , , with the wavelength of and natural width of . The temperature of the atomic cloud in a magneto-optical trap (MOT) was at the lifetime of and the number of atoms . Approximately 1 % of atoms from the MOT have been reloade...

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Veröffentlicht in:Quantum electronics (Woodbury, N.Y.) N.Y.), 2014-06, Vol.44 (6), p.515-520
Hauptverfasser: Sukachev, D.D., Kalganova, E.S., Sokolov, A.V., Fedorov, S.A., Vishnyakova, G.A., Akimov, A.V., Kolachevsky, N.N., Sorokin, V.N.
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Sprache:eng
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Zusammenfassung:Secondary laser cooling has been realised on the weak dipole transition , , , , with the wavelength of and natural width of . The temperature of the atomic cloud in a magneto-optical trap (MOT) was at the lifetime of and the number of atoms . Approximately 1 % of atoms from the MOT have been reloaded to an optical dipole trap and to one-dimensional optical lattice at the wavelength of . The atom lifetime in the optical lattice was . We propose to employ thulium atoms captured in an optical lattice as an optical frequency reference.
ISSN:1063-7818
1468-4799
DOI:10.1070/QE2014v044n06ABEH015392