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Hyperfine structure in the 4p55d states of Kr83

Rupesh Silwal and J. R. Brandenberger

  • Department of Physics, Lawrence University, Appleton, Wisconsin 54912, USA

Phys. Rev. A 73, 032508 – Published 15 March, 2006

DOI: https://doi.org/10.1103/PhysRevA.73.032508

Abstract

Hyperfine splittings in the 4d1, 4d3, 4d4, and 4d5 states of the 4p55d configuration of Kr83(I=92) have been measured using two-step laser excitation. The corresponding hyperfine coupling constants A and B are negative (with one exception) and range from 400to+85MHz.

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References (13)

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  4. The isotopically enriched krypton gas was supplied by Isotec, Inc.

  5. The 30MHz oscillator used here is a variant on the design discussed in W. E. Bell, A. L. Bloom, and J. Lynch, Rev. Sci. Instrum. 32, 688 (1961).
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  7. All wavelengths quoted in this paper are measured in air.

  8. By a v0 velocity group, we mean Kr83 atoms whose velocity components parallel to the laser beams are essentially zero.

  9. The scanning of an external cavity diode laser can exhibit small nonuniformities or nonlinearities due to (i) competition between the resonances of the laser’s internal and external cavities and (ii) nonlinearity in the expansion of the piezoelectric crystal that tunes the external cavity.

  10. These commercially available diode lasers are manufactured or distributed by Sharp, Sanyo, Toptica, Roithner, Thorlabs, and Optima Precision.

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