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1
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0000943624
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Pulse propagation and many-body effects in semiconductor four-wave mixing
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A. Schulze, A. Knorr, and S. W. Koch, "Pulse propagation and many-body effects in semiconductor four-wave mixing," Phys. Rev. B 51, 10601-10609 (1995).
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Phys. Rev. B
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Schulze, A.1
Knorr, A.2
Koch, S.W.3
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2
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0031125851
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Interplay of optical dephasing and pulse propagation in semiconductors
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S. Hughes, A. Knorr, and S. W. Koch, "Interplay of optical dephasing and pulse propagation in semiconductors," J. Opt. Soc. Am. B 14, 754-760 (1997).
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(1997)
J. Opt. Soc. Am. B
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Hughes, S.1
Knorr, A.2
Koch, S.W.3
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3
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0000720233
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Polarization decay in ultrafast collinear nondegenerate four-wave mixing in a semiconductor amplifier
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S. Hughes, "Polarization decay in ultrafast collinear nondegenerate four-wave mixing in a semiconductor amplifier," Opt. Lett. 23, 948-950 (1998).
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Opt. Lett.
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Hughes, S.1
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4
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0029184894
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Filamentation and beam propagation in broad-area semiconductor lasers
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O. Hess, S. W. Koch, and J. V. Moloney, "Filamentation and beam propagation in broad-area semiconductor lasers," IEEE J. Quantum Electron. 31, 35-43 (1995).
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(1995)
IEEE J. Quantum Electron.
, vol.31
, pp. 35-43
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Hess, O.1
Koch, S.W.2
Moloney, J.V.3
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5
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11744315558
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Maxwell-Bloch equations for spatially inhomogeneous semiconductor laser. II. Spatiotemporal dynamics
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O. Hess and T. Kühn, "Maxwell-Bloch equations for spatially inhomogeneous semiconductor laser. II. Spatiotemporal dynamics," Phys. Rev. A 54, 3360-3368 (1996).
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(1996)
Phys. Rev. A
, vol.54
, pp. 3360-3368
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Hess, O.1
Kühn, T.2
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6
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0030578788
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Complex spatio-temporal dynamics in the nearfield of a broad-area semiconductor laser
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I. Fischer, O. Hess, W. Elsässer, and E. Göbel, "Complex spatio-temporal dynamics in the nearfield of a broad-area semiconductor laser," Europhys. Lett. 35, 579-584 (1996).
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(1996)
Europhys. Lett.
, vol.35
, pp. 579-584
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Fischer, I.1
Hess, O.2
Elsässer, W.3
Göbel, E.4
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7
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34248651615
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Effective Bloch equations for semiconductors
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M. Lindberg and S. W. Koch, "Effective Bloch equations for semiconductors," Phys. Rev. B 33, 3342-3350 (1988).
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(1988)
Phys. Rev. B
, vol.33
, pp. 3342-3350
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Lindberg, M.1
Koch, S.W.2
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8
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0001767809
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Semiconductor laser theory with many-body effects
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H. Haug and S. W. Koch, "Semiconductor laser theory with many-body effects," Phys. Rev. A 39, 1887-1898 (1989).
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(1989)
Phys. Rev. A
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Haug, H.1
Koch, S.W.2
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9
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17544371067
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Maxwell-Bloch equations for spatially inhomogeneous semiconductor lasers. I. Theoretical description
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O. Hess and T. Kuhn, "Maxwell-Bloch equations for spatially inhomogeneous semiconductor lasers. I. Theoretical description," Phys. Rev. A 54, 3347-3359 (1996).
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(1996)
Phys. Rev. A
, vol.54
, pp. 3347-3359
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Hess, O.1
Kuhn, T.2
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10
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0032023032
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Nonequilibrium spatio-temporal dynamics of the Wigner-distributions in broad-area semiconductor lasers
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E. Gehrig and O. Hess, "Nonequilibrium spatio-temporal dynamics of the Wigner-distributions in broad-area semiconductor lasers," Phys. Rev. A 57, 2150-2163 (1998).
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(1998)
Phys. Rev. A
, vol.57
, pp. 2150-2163
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Gehrig, E.1
Hess, O.2
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11
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0029709958
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Spatio-temporal dynamics of semiconductor lasers: Theory, modeling and analysis
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O. Hess and T. Kuhn, "Spatio-temporal dynamics of semiconductor lasers: theory, modeling and analysis," Prog. Quantum Electron. 20, 85-179 (1996).
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(1996)
Prog. Quantum Electron.
, vol.20
, pp. 85-179
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Hess, O.1
Kuhn, T.2
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12
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0010850958
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Microscopic theory of the optical band edge nonlinearities
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H. Haug, ed. Academic, New York
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H. Haug, "Microscopic theory of the optical band edge nonlinearities," in Optical Nonlinearities and Instabilities in Semiconductors, H. Haug, ed. (Academic, New York, 1988), pp. 53-81.
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(1988)
Optical Nonlinearities and Instabilities in Semiconductors
, pp. 53-81
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Haug, H.1
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16
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0023983289
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Nonlinear optics and the Mott transition in semiconductors
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R. Zimmermann, "Nonlinear optics and the Mott transition in semiconductors," Phys. Status Solidi B 146, 371-384 (1988).
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(1988)
Phys. Status Solidi B
, vol.146
, pp. 371-384
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Zimmermann, R.1
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17
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84894396642
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note
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Although the self-focusing processes may in general depend on the particular spatial shape of the input pulses and their power densities, the conditions assumed here can be considered typical; i.e., within a large variation of input intensities, only minor quantitative changes in the behavior have been observed in the simulations.
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