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See, e.g
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See, e.g., R. Butté, G. Delalleau, A I. Tartakovskii, M S. Skolnick, V N. Astratov, Phys. Rev. B65, 205310 (2002).
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18
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85038309238
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In our previous work in Ref., performed on a 1λ cavity with, Bragg mirrors but without control of electric field, residual built-in fields led to partial suppression of photoluminescence
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In our previous work in Ref. 8, performed on a 1λ cavity with p, n Bragg mirrors but without control of electric field, residual built-in fields led to partial suppression of photoluminescence.
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19
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33646657680
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D A B. Miller, D S. Chemla, T C. Damen, A C. Gossard, W. Wiegmann, and T H. Wood, Phys. Rev. B32, 1043 (1985).
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Wood, T.H.6
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21
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85038308254
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Correcting for the strongly energy-dependent transmission factor for double resonance nevertheless leads to Raman cross sections very similar to those presented here
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Correcting for the strongly energy-dependent transmission factor for double resonance nevertheless leads to Raman cross sections very similar to those presented here.
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22
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0001148399
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In this reference resonance was maintained by temperature tuning, enabling (formula presented) to be determined directly at each field
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T A. Fisher, Phys. Rev. B51, 2600 (1995). In this reference resonance was maintained by temperature tuning, enabling (formula presented) to be determined directly at each field.
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Fisher, T.A.1
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23
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85038272349
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It is estimated in Ref., that the maximum coupling occurs for in-plane wave vectors (formula presented)
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It is estimated in Ref. 13 that the maximum coupling occurs for in-plane wave vectors (formula presented)
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-
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24
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0001757460
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The dispersion in LO phonon energy over this range of, is ∼0.1 meV, less than the experimental resolution, see, e.g
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The dispersion in LO phonon energy over this range of k is ∼0.1 meV, less than the experimental resolution, see, e.g., Fasol, Phys. Rev. B38, 6056 (1988).
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26
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0001508844
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Phys. Rev. BR. Houdré, C. Weisbuch, R P. Stanley, U. Oesterle, and M. Ilegems, 61, R13 333 (2000);
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29
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85038323878
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In Ref., the peak at the exciton energy was observed only for incoming resonance and not for the outgoing process
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In Ref. 8 the peak at the exciton energy was observed only for incoming resonance and not for the outgoing process.
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