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1
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Benson, E., Fortin, E. and Mysyrowicz, A., Phys. Status Solidi (b) 191, 1995, 345.
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Benson, E.1
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0000070742
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Mysyrowicz, A., Benson, E. and Fortin, E., Phys. Rev. Lett. 77, 1996, 896.
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Phys. Rev. Lett.
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Mysyrowicz, A., Snoke, D. and Wolfe, J.P., Phys. Status Solidi (b) 159, 1990, 387.
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Phys. Status Solidi (B)
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Wolfe, J.P.3
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5
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0000523486
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Kavoulakis, G.M., Baym, G. and Wolfe, J.P., Phys. Rev. B53, 1996, 7227.
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6
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Snoke, D., Wolfe, J.P. and Mysyrowicz, A., Phys. Rev. B41, 1990, 11171.
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Phys. Rev.
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Snoke, D.1
Wolfe, J.P.2
Mysyrowicz, A.3
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9
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30244472614
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(Edited by D.J. Lockwood), World Scientific, Singapore
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Kopelevich, G.A. and Tikhodeev, S.G., Proc. 22nd Conf. Phys. Semicond. (Edited by D.J. Lockwood), p. 61. World Scientific, Singapore, 1995; Kopelevich, G.A., Gippius, N.A. and Tikhodeev, S.G., Solid State Commun. 99, 1996, 93.
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10
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0030191877
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Kopelevich, G.A. and Tikhodeev, S.G., Proc. 22nd Conf. Phys. Semicond. (Edited by D.J. Lockwood), p. 61. World Scientific, Singapore, 1995; Kopelevich, G.A., Gippius, N.A. and Tikhodeev, S.G., Solid State Commun. 99, 1996, 93.
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Kopelevich, G.A.1
Gippius, N.A.2
Tikhodeev, S.G.3
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11
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85033112199
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note
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To be more precise, acoustic phonons are generated in the crystal during ortho-to para-exciton conversion of the cold probe excitons. However, most of these probe-produced acoustic phonons are generated in the bulk; consequently they scatter excitons nearly isotropically, not preferentially towards the rear surface.
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12
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4243988677
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Trauernicht, D., Wolfe, J.P. and Mysyrowicz, A., Phys. Rev. Lett. 43, 1979, 1123.
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Trauernicht, D.1
Wolfe, J.P.2
Mysyrowicz, A.3
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13
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4243988677
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Mysyrowicz, A., Hulin, D. and Antonetti, A., Phys. Rev. Lett. 43, 1979, 1123.
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Phys. Rev. Lett.
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Mysyrowicz, A.1
Hulin, D.2
Antonetti, A.3
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14
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0001226222
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Snoke, D.W., Shields, A.J. and Cardona, M., Phys. Rev. B45, 1992, 11693.
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Phys. Rev.
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Snoke, D.W.1
Shields, A.J.2
Cardona, M.3
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15
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30244549576
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(Edited by Griffin, Snoke and Stringari), Cambridge University Press
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Mysyrowicz, A., in Bose-Einstein Condensation (Edited by Griffin, Snoke and Stringari), p. 346. Cambridge University Press, 1995.
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Bose-Einstein Condensation
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Mysyrowicz, A.1
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17
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85033113495
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note
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The lack of a significant raise of lattice temperature (hot spot) at the front surface is ruled out by the fact that the spectral position of the exciton, which depends on lattice temperature remains unchanged during the excitation laser pulse [3, 5].
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