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2008
DOI: 10.1016/j.jlumin.2007.06.003
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Temperature dependence of excitonic emission in cubic CdSe thin film

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Cited by 27 publications
(21 citation statements)
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“…This elevated E exc (0) compared with the bulk-like ZB CdSe epilayers (1.739 eV) 47 is due to increased quantum confinement effects. Further, we obtain a ep = 18.2 ± 2.8 meV and Θ = 36 ± 0.4 K. Chia et al 47 calculated a ep = 21 meV for bulk-like ZB CdSe epilayers. This shows that the increased confinement in the NPLs has reduced the average exciton-phonon coupling, which is also evident from the significant reduction in average phonon temperature of 305 K in bulk ZB CdSe.…”
Section: −T/τ2mentioning
confidence: 95%
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“…This elevated E exc (0) compared with the bulk-like ZB CdSe epilayers (1.739 eV) 47 is due to increased quantum confinement effects. Further, we obtain a ep = 18.2 ± 2.8 meV and Θ = 36 ± 0.4 K. Chia et al 47 calculated a ep = 21 meV for bulk-like ZB CdSe epilayers. This shows that the increased confinement in the NPLs has reduced the average exciton-phonon coupling, which is also evident from the significant reduction in average phonon temperature of 305 K in bulk ZB CdSe.…”
Section: −T/τ2mentioning
confidence: 95%
“…49 Furthermore, with increasing temperature, we also have a substantial reduction in the PL intensity as the excitons are trapped in the nonradiative centers, likely at NPL surfaces and dissociate into the continuum states. The integrated intensity of the PL spectra with varying temperatures is given by 47,52 IðTÞ…”
Section: −T/τ2mentioning
confidence: 99%
“…The coupling to optical modes tends to increase with A and then saturate for large platelet areas towards values reported by Chia et al for laterally infinite MBE grown CdSe epilayers (≈20 meV). 67 As the Fröhlich interaction is considered the dominating mechanism 42 for the LO phonon coupling in polar semiconductor nano-structures we briefly investigate whether this can explain the observed complicated behavior directly. The corresponding interaction potential 59…”
Section: Nanoscale Papermentioning
confidence: 99%
“…One more anomalous feature of the DPL band can be seen from this figure. In particular, a pronounced redshift of the DPL band is observed for all samples ( Figure 9 a), contrary to the well-established PL behavior upon decreasing temperature, which includes blue shift and narrowing of PL bands [ 55 , 56 ]. We attribute this rather anomalous behavior to the suppressed thermal occupation of higher-energy trap states, resulting in a lower average energy of the occupied trap states at lower temperature, and thus a lower energy of the PL maximum.…”
Section: Resultsmentioning
confidence: 58%