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The nonlinear signal is also known in the literature as picosecond excitation-correlation (PEC) or intensity correlation luminescence.
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30244575132
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note
-
The 'dark' exciton state at K also may be considered to be a linear combination of Slater determinant crystal states with a conduction band electron at K and a valence band vacancy at K - k for all possible k. We expect that the saturation value for large K exciton density imposed by the fermi exclusion is much larger than the occupancy of dark excitons at K in our experiments. This may be justified on the grounds that the excited dark excitons distribute over the K space with a 2D degeneracy of motion whereas those at K ≈ 0 have a much smaller phase space available.
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-
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28
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0000905694
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-
x can be found in Lee, J., Koteles, E.S. and Vassell, M.O., Phys. Rev. B, 33, 1986, 5512; Chen, Y.J., Koteles, E.S., Lee, J. and Elman, B.S., Proc. SPIE, 792, 1987, 162. At very low temperatures, the exciton lifetime has a different form governed by intrinsic radiative lifetime, as obtained by Andreani, L.C., Tassone, F. and Bassani, F., Solid State Commun., 77, 1991, 641.
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Phys. Rev. B
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84950548003
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x can be found in Lee, J., Koteles, E.S. and Vassell, M.O., Phys. Rev. B, 33, 1986, 5512; Chen, Y.J., Koteles, E.S., Lee, J. and Elman, B.S., Proc. SPIE, 792, 1987, 162. At very low temperatures, the exciton lifetime has a different form governed by intrinsic radiative lifetime, as obtained by Andreani, L.C., Tassone, F. and Bassani, F., Solid State Commun., 77, 1991, 641.
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Proc. SPIE
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Koteles, E.S.2
Lee, J.3
Elman, B.S.4
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0026119227
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x can be found in Lee, J., Koteles, E.S. and Vassell, M.O., Phys. Rev. B, 33, 1986, 5512; Chen, Y.J., Koteles, E.S., Lee, J. and Elman, B.S., Proc. SPIE, 792, 1987, 162. At very low temperatures, the exciton lifetime has a different form governed by intrinsic radiative lifetime, as obtained by Andreani, L.C., Tassone, F. and Bassani, F., Solid State Commun., 77, 1991, 641.
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