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edited by M. Evans and S. Kielich, Wiley, New York
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edited by D.H.E. Dubin and D. Schneider American Institute of Physics, New York
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V. A. Sautenkov, M. D. Lukin, C. J. Bednar, I. Novikova, E. Mikhailov, M. Fleischhauer, V. L. Velichansky, G. R. Welch, and M. O. Scully, Phys. Rev. A 62, 023810 (2000); M. Fleischhauer, A. B. Matsko, and M. O. Scully, Phys. Rev. A 62, 013808 (2000).
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V. A. Sautenkov, M. D. Lukin, C. J. Bednar, I. Novikova, E. Mikhailov, M. Fleischhauer, V. L. Velichansky, G. R. Welch, and M. O. Scully, Phys. Rev. A 62, 023810 (2000); M. Fleischhauer, A. B. Matsko, and M. O. Scully, Phys. Rev. A 62, 013808 (2000).
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0004180692
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Springer-Verlag, Berlin
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Here alignment designates the second (quadrupole) polarization moment, and orientation designates the first (dipole) polarization moment; see E. B. Alexandrov, M. P. Chaika, and G. I. Kvostenko, Interference of Atomic States (Springer-Verlag, Berlin, 1993).
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Interference of Atomic States
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Alexandrov, E.B.1
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14
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0002696446
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USSR
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This is because for closed transitions, the axis of dichroism corresponding to smaller absorption is initially parallel to the direction of the pump light polarization for F → F - 1, F transitions (atoms are pumped into a dark state), and perpendicular to the pump light polarization for F → F + 1 transitions (atoms are pumped into a bright state with greater absorption compared to the unpolarized state [A. P. Kazantsev, V. S. Smirnov, A. M. Tumaikin, and I. A. Yagofarov, Opt. Spectrosc. (USSR) 57, 116 (1984)]).
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Kazantsev, A.P.1
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Yagofarov, I.A.4
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0009680173
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USSR
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In our calculations, a density matrix is written for Zeeman sublevels of each ground state hyperfine level and for those of all the excited states accessible via optical transitions from this hyperfine level. The effects of repopulation pumping are included in the calculations. These calculations are based on principles similar to those applied in M. G. Kozlov, Opt. Spectrosc. (USSR) 67, 789 (1989); S. V. Fomichev, J. Phys. B 24, 4695 (1991); G. Nienhuis and F. Schuller, Opt. Commun. 151, 40 (1998), and references therein.
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Kozlov, M.G.1
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0012633062
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In our calculations, a density matrix is written for Zeeman sublevels of each ground state hyperfine level and for those of all the excited states accessible via optical transitions from this hyperfine level. The effects of repopulation pumping are included in the calculations. These calculations are based on principles similar to those applied in M. G. Kozlov, Opt. Spectrosc. (USSR) 67, 789 (1989); S. V. Fomichev, J. Phys. B 24, 4695 (1991); G. Nienhuis and F. Schuller, Opt. Commun. 151, 40 (1998), and references therein.
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Fomichev, S.V.1
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17
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0032068485
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and references therein
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In our calculations, a density matrix is written for Zeeman sublevels of each ground state hyperfine level and for those of all the excited states accessible via optical transitions from this hyperfine level. The effects of repopulation pumping are included in the calculations. These calculations are based on principles similar to those applied in M. G. Kozlov, Opt. Spectrosc. (USSR) 67, 789 (1989); S. V. Fomichev, J. Phys. B 24, 4695 (1991); G. Nienhuis and F. Schuller, Opt. Commun. 151, 40 (1998), and references therein.
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Schuller, F.2
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0017503039
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Under the stated conditions, this formula is a good approximation of the expression obtained from dressed state considerations for a two-level atom in, e.g., C. Cohen-Tannoudji, Metrologia 13, 161 (1977).
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Cohen-Tannoudji, C.1
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0034543239
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OSA Technical Digest Optical Society of America, Washington, D.C.
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D. Budker, R. Y. Chiao, D. S. Hsiung, S. M. Rochester, and V. V. Yashchuk, in Quantum Electronics and Laser Science, OSA Technical Digest (Optical Society of America, Washington, D.C., 2000), p. 252.
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Quantum Electronics and Laser Science
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Budker, D.1
Chiao, R.Y.2
Hsiung, D.S.3
Rochester, S.M.4
Yashchuk, V.V.5
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0039615801
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L. M. Barkov, M. S. Zolotorev, and D. Melik-Pashayev, Sov. JETP Pis'ma 48, 144 (1988); L. M. Barkov, D. A. Melik-Pashayev, and M. S. Zolotorev, Opt. Commun. 70, 467 (1989).
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Barkov, L.M.1
Zolotorev, M.S.2
Melik-Pashayev, D.3
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L. M. Barkov, M. S. Zolotorev, and D. Melik-Pashayev, Sov. JETP Pis'ma 48, 144 (1988); L. M. Barkov, D. A. Melik-Pashayev, and M. S. Zolotorev, Opt. Commun. 70, 467 (1989).
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