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0 = cos 2∈ sin 2α. [30] 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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Polarization of Light
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0017503039
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0 = cos 2∈ sin 2α. [30] 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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0004180692
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0023844385
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Our calculations are based on principles similar to those applied in F. Schuller, M.J.D. Macpherson, and D.N. Stacey, Physica C 147, 321 (1987); F. Schuller, M.J.D. Macpherson, and D.N. Stacey, Opt. Commun. 71, 61 (1989); M.G. Kozlov, Opt. Spectrosc. 67, 789 (1989); S.V. Fomichev, J. Phys. B 24, 4695 (1991); K.P. Zetie, R.B. Warrington, M.J.D. Macpherson, D.N. Stacey, and F. Schuller, Opt. Commun. 91, 210 (1992); F. Schuller, D.N. Stacey, R.B. Warrington, and K.P. Zetie, J. Phys. B 28, 3783 (1995); G. Nienhuis and F. Schuller, Opt. Commun. 151, 40 (1998).
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0024657265
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Our calculations are based on principles similar to those applied in F. Schuller, M.J.D. Macpherson, and D.N. Stacey, Physica C 147, 321 (1987); F. Schuller, M.J.D. Macpherson, and D.N. Stacey, Opt. Commun. 71, 61 (1989); M.G. Kozlov, Opt. Spectrosc. 67, 789 (1989); S.V. Fomichev, J. Phys. B 24, 4695 (1991); K.P. Zetie, R.B. Warrington, M.J.D. Macpherson, D.N. Stacey, and F. Schuller, Opt. Commun. 91, 210 (1992); F. Schuller, D.N. Stacey, R.B. Warrington, and K.P. Zetie, J. Phys. B 28, 3783 (1995); G. Nienhuis and F. Schuller, Opt. Commun. 151, 40 (1998).
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0023844385
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Our calculations are based on principles similar to those applied in F. Schuller, M.J.D. Macpherson, and D.N. Stacey, Physica C 147, 321 (1987); F. Schuller, M.J.D. Macpherson, and D.N. Stacey, Opt. Commun. 71, 61 (1989); M.G. Kozlov, Opt. Spectrosc. 67, 789 (1989); S.V. Fomichev, J. Phys. B 24, 4695 (1991); K.P. Zetie, R.B. Warrington, M.J.D. Macpherson, D.N. Stacey, and F. Schuller, Opt. Commun. 91, 210 (1992); F. Schuller, D.N. Stacey, R.B. Warrington, and K.P. Zetie, J. Phys. B 28, 3783 (1995); G. Nienhuis and F. Schuller, Opt. Commun. 151, 40 (1998).
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Our calculations are based on principles similar to those applied in F. Schuller, M.J.D. Macpherson, and D.N. Stacey, Physica C 147, 321 (1987); F. Schuller, M.J.D. Macpherson, and D.N. Stacey, Opt. Commun. 71, 61 (1989); M.G. Kozlov, Opt. Spectrosc. 67, 789 (1989); S.V. Fomichev, J. Phys. B 24, 4695 (1991); K.P. Zetie, R.B. Warrington, M.J.D. Macpherson, D.N. Stacey, and F. Schuller, Opt. Commun. 91, 210 (1992); F. Schuller, D.N. Stacey, R.B. Warrington, and K.P. Zetie, J. Phys. B 28, 3783 (1995); G. Nienhuis and F. Schuller, Opt. Commun. 151, 40 (1998).
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J. Phys. B
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Our calculations are based on principles similar to those applied in F. Schuller, M.J.D. Macpherson, and D.N. Stacey, Physica C 147, 321 (1987); F. Schuller, M.J.D. Macpherson, and D.N. Stacey, Opt. Commun. 71, 61 (1989); M.G. Kozlov, Opt. Spectrosc. 67, 789 (1989); S.V. Fomichev, J. Phys. B 24, 4695 (1991); K.P. Zetie, R.B. Warrington, M.J.D. Macpherson, D.N. Stacey, and F. Schuller, Opt. Commun. 91, 210 (1992); F. Schuller, D.N. Stacey, R.B. Warrington, and K.P. Zetie, J. Phys. B 28, 3783 (1995); G. Nienhuis and F. Schuller, Opt. Commun. 151, 40 (1998).
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Our calculations are based on principles similar to those applied in F. Schuller, M.J.D. Macpherson, and D.N. Stacey, Physica C 147, 321 (1987); F. Schuller, M.J.D. Macpherson, and D.N. Stacey, Opt. Commun. 71, 61 (1989); M.G. Kozlov, Opt. Spectrosc. 67, 789 (1989); S.V. Fomichev, J. Phys. B 24, 4695 (1991); K.P. Zetie, R.B. Warrington, M.J.D. Macpherson, D.N. Stacey, and F. Schuller, Opt. Commun. 91, 210 (1992); F. Schuller, D.N. Stacey, R.B. Warrington, and K.P. Zetie, J. Phys. B 28, 3783 (1995); G. Nienhuis and F. Schuller, Opt. Commun. 151, 40 (1998).
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Our calculations are based on principles similar to those applied in F. Schuller, M.J.D. Macpherson, and D.N. Stacey, Physica C 147, 321 (1987); F. Schuller, M.J.D. Macpherson, and D.N. Stacey, Opt. Commun. 71, 61 (1989); M.G. Kozlov, Opt. Spectrosc. 67, 789 (1989); S.V. Fomichev, J. Phys. B 24, 4695 (1991); K.P. Zetie, R.B. Warrington, M.J.D. Macpherson, D.N. Stacey, and F. Schuller, Opt. Commun. 91, 210 (1992); F. Schuller, D.N. Stacey, R.B. Warrington, and K.P. Zetie, J. Phys. B 28, 3783 (1995); G. Nienhuis and F. Schuller, Opt. Commun. 151, 40 (1998).
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84889139800
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note
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In this work, a vapor cell with no antirelaxation coating was used. Thus atomic polarization was destroyed by collisions with the cell wall, and so could be ignored in the pumping term.
-
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56
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84889161126
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note
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The system of equations is solved numerically using code written in MATHEMATICA, which calls C-language routines employing SPARSE, a sparse matrix package by K. S. Kundert and A. Sangiovanni-Vincentelli, University of California, Berkeley (April 1988).
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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 Conference, OSA Technical Digest (Optical Society of America, Washington, DC, 2000), p. 252.
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Budker, D.1
Chiao, R.Y.2
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Rochester, S.M.4
Yashchuk, V.V.5
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