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33646656053
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note
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In the PL spectra of some of the samples, emission from the excited exciton state is also visible, with an intensity depending on the confinement energy, i.e., the excited-state splitting. State filling effects are ruled out by the low excitation intensity. This emission appears to be due to a confinement dependent inhibition of the relaxation into the ground state (phonon bottleneck). In fact, the excited state emission vanishes for temperatures above 80 K, for which phonon assisted excitation into higher excited-states and subsequent relaxation is possible, as reported in Ref. 29.
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14
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19
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33646637660
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note
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Since the oscillator strength of the |x〉 |y〉 transitions are differing slightly, the excited exciton state is not purely circular polarized, but the consequent alteration of the FWM signal is not significant.
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20
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0001170670
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33646647738
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note
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The two fine-structure split states can have slightly different dephasing rates. The smaller the fine-structure splitting gets, the less significant is the difference in the decay rates, so that it can be neglected in the analysis of the beat structures.
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22
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33646658885
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note
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T considering the effect of the Indiffusion based annealing on the QD shape.
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23
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0000193342
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24
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33646648967
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note
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B>0.
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28
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0036544178
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30
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0035099783
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J.J. Finley, A.D. Ashmore, A. Lemaître, D.J. Mowbray, M.S. Skolnick, I.E. Itskevich, P.A. Maksym, M. Hopkinson, and T.F. Krauss, Phys. Rev. B 63, 073307 (2001).
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