-
2
-
-
85015726585
-
-
note
-
It is assumed that Γ is much less than the linewidth of the atomic transition, and also that the lower level of the transition is unoccupied.
-
-
-
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5
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4243834860
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A. E. Siegman, Phys. Rev. A 39, 1253 (1989); 39, 1264 (1989) .
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7
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6144227388
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M. A. van Eijkelenborg, Å. M. Lindberg, M. S. Thijssen, and J. P. Woerdman, Phys. Rev. Lett. 77, 4314 (1996).
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Van Eijkelenborg, M.A.1
Lindberg, Å.M.2
Thijssen, M.S.3
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8
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0001336747
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M. Brunel, G. Ropars, A. Le Floch, and F. Bretenaker, Phys. Rev. A 55, 4563 (1997).
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Phys. Rev. A
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Brunel, M.1
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Bretenaker, F.4
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16
-
-
85015721588
-
-
note
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ll, and take the real part.
-
-
-
-
17
-
-
4243604066
-
-
note
-
2/δω. The linewidth differs from the Schawlow-Townes value [Eq. (1)] by a factor 2K. The extra factor 2 arises from the suppression of amplitude fluctuations in the nonlinear regime above the laser threshold, as explained by P. Goldberg, P. W. Milonni, and B. Sundaram, Phys. Rev. A 44, 1969 (1991).
-
-
-
-
18
-
-
85015740733
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-
note
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Ω,Γ. The distribution P(Ω,Γ) of the lasing mode was calculated in Ref. [14].
-
-
-
-
20
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-
0000031438
-
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F. von Oppen, Phys. Rev. Lett. 73, 798 (1994); Phys. Rev. E 51, 2647 (1995).
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22
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36149016205
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6 for T ≪ 1. See H. A. Bethe, Phys. Rev. 66, 163 (1944).
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Bethe, H.A.1
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23
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11944268987
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Alt, H.1
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Schardt, P.7
Weidenmüller, H.A.8
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24
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3142730527
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25
-
-
85015794587
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-
note
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2]exp(-π/2κ) for T ≪ 1.
-
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27
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0001497834
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R. A. Janik, W. Nörenberg, M. A. Nowak, G. Papp, and I. Zahed, Phys. Rev. E 60, 2699 (1999).
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28
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0032486186
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Gmachl, C.1
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Stone, A.D.5
Faist, J.6
Sivco, D.L.7
Cho, A.Y.8
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