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84894396090
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note
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For polarization along the growth direction, the fundamental mode of the cavity has the same dispersion as a free photon, and a situation similar to that of Ref. 7 would result.
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21
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84894398680
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note
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14). For the sake of simplicity we have avoided their introduction, which does not alter any of the physically significant effect.
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24
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0001607396
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V. Savona, F. Tassone, C. Piermarocchi, A. Quattropani, and P. Schwendimann, Phys. Rev. B 53, 13051 (1996).
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Schwendimann, P.5
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26
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0001523741
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This may lead to an additional luminescence band between the Raby split lines [eee also the discussion in R. Houdre, R. P. Stanley, and M. Ilegems, Phys. Rev. A 53, 2711 (1996)]. A dark state partially activated by mixing with an optically active one may also be responsible for the so called weak-coupling component observed in resonant Raman scattering [A. Fainstein, B. Jusserand, and V. Thierry-Mieg, Phys. Rev. Lett. 78, 1576 (1997)].
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Phys. Rev. A
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0031076575
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This may lead to an additional luminescence band between the Raby split lines [eee also the discussion in R. Houdre, R. P. Stanley, and M. Ilegems, Phys. Rev. A 53, 2711 (1996)]. A dark state partially activated by mixing with an optically active one may also be responsible for the so called weak-coupling component observed in resonant Raman scattering [A. Fainstein, B. Jusserand, and V. Thierry-Mieg, Phys. Rev. Lett. 78, 1576 (1997)].
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Phys. Rev. Lett.
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Fainstein, A.1
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28
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0009365437
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Here we assume that the structural quality is high enough to preclude such a localization along the cavity axis. See also the discussion in H. Cao, S. Pau, Y. Yamamoto, and G. Bjork, Phys. Rev. B 54, 8083 (1996).
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30
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84894394305
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note
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Short-wavelength phonons as well as interface and confined-phonon modes associated with the multiple-quantum-well structure may lead to a partial mixing of the b states because they are coupled to excitons in different wells.
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32
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0030566529
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A discussion of this issue, also in relation to the motional narrowing considered in D. M. Whittaker, P. Kinsler, T. A. Fisher, M. S. Skolnick, A. Armitage, A. M. Afshar, M. D. Sturge, and J. S. Roberts, Phys. Rev. Lett. 77, 4792 (1996), will be given elsewhere [V. M. Agranovich, G. C. La Rocca, and F. Bassani, Phys. Rev. Lett. (to be published)].
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Whittaker, D.M.1
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Afshar, A.M.6
Sturge, M.D.7
Roberts, J.S.8
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33
-
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84894400997
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to be published
-
A discussion of this issue, also in relation to the motional narrowing considered in D. M. Whittaker, P. Kinsler, T. A. Fisher, M. S. Skolnick, A. Armitage, A. M. Afshar, M. D. Sturge, and J. S. Roberts, Phys. Rev. Lett. 77, 4792 (1996), will be given elsewhere [V. M. Agranovich, G. C. La Rocca, and F. Bassani, Phys. Rev. Lett. (to be published)].
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Phys. Rev. Lett.
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Agranovich, V.M.1
La Rocca, G.C.2
Bassani, F.3
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34
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84894389486
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note
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It would be interesting to calculate the biexciton properties in the presence of the cavity along the lines followed in Ref. 7 for a free quantum well.
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35
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59049093019
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Pergamon, London, Sect. 45
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