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In most cases N is large enough that ΓN ≫ γ and the line width is given by ≈αNg2R/c. However, the more correct form given by Eqs, 2, 3 is instructive as it shows the line width is lower bounded by γ. The author wishes to thank A. Svidzinsky and M.S. Zubairy for useful discussions on this point
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2R/c. However, the more correct form given by Eqs. (2), (3) is instructive as it shows the line width is lower bounded by γ. The author wishes to thank A. Svidzinsky and M.S. Zubairy for useful discussions on this point.
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W. Chow, M. Scully, and J. Stoner, Jr., Phys. Rev. A 11, 1380 (1975).
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Theory: M. Scully
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Theory: M. Scully, Phys. Rev. Lett. 55, 2802 (1985).
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Experiment: M. Winters, J. Hall, and P. Toschek, Phys. Rev. Lett. 65, 3116 (1990).
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Quantum Statistical Theories of Spontaneous Emission
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Agarwal, G.1
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16
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34249654946
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Cooperative Spontaneous Emission as a Many Body Eigenstable Problem
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to be published
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A. Svidzinsky, M. Scully, and R. Glauber, "Cooperative Spontaneous Emission as a Many Body Eigenstable Problem," to be published.
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Svidzinsky, A.1
Scully, M.2
Glauber, R.3
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17
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34249677200
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A. Svidzinsky and M. Scully, to be published. See also A. Gorshkov, A. André, M. Fleishauer, A. Sorensen, and M. Lukin, to be published.
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A. Svidzinsky and M. Scully, to be published. See also A. Gorshkov, A. André, M. Fleishauer, A. Sorensen, and M. Lukin, to be published.
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34249679008
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We note the close correspondence between incoherent Raman and coherent Raman (CARS) scattering in the present context; See the MOS lecture notes on the subject available upon request
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We note the close correspondence between incoherent Raman and coherent Raman (CARS) scattering in the present context; See the MOS lecture notes on the subject available upon request.
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