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To obtain this result, we used the measured spectrometer response function and assumed that the excitonic ground-state line shape is Lorentzian, as observed for the excited states (left inset, Fig. 2)
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To obtain this result, we used the measured spectrometer response function and assumed that the excitonic ground-state line shape is Lorentzian, as observed for the excited states (left inset, Fig. 2).
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22
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36549092968
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In this sense our localized exciton system is qualitatively different from that examined in the earlier linewidth studies (1-5). This difference arises from the use of growth interrupts at the interfaces in our samples, which completely changes the spectral and spatial distribution of the localized states [see, for example, D. Gammon et al., Appl. Phys. Lett. 57, 2710 (1990)].
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9344226965
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note
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-1 for a 28-nm quantum well (23).
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28
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0000562906
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0001039741
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V. Srinivas, Y. J. Chen, C. E. C. Wood, Phys. Rev. B 46, 10193 (1992); D. Gammon, S. Rudin, T. L. Reinecke, D. S. Katzer, C. S. Kyona, ibid. 51, 16785 (1995).
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Gammon, D.1
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Kyona, C.S.5
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9344232134
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This research was funded in part by the office of Naval Research
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This research was funded in part by the office of Naval Research
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