2017
DOI: 10.1364/ome.7.000808
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Variation of phonon coupling factors in the photoluminescence of cadmium telluride by variable excitation power

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Cited by 4 publications
(2 citation statements)
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“…With a rise in excitation power density, a greater number of electron-hole pairs are generated, and the electrons and holes located at k ≠ 0 also recombine, thus contributing to the observed peak width [48]. This phenomenon is observed in numerous materials [49,50]. Figure 6 illustrates the evolution of the PL spectra at 17 K for various power excitation densities.…”
Section: Resultsmentioning
confidence: 98%
“…With a rise in excitation power density, a greater number of electron-hole pairs are generated, and the electrons and holes located at k ≠ 0 also recombine, thus contributing to the observed peak width [48]. This phenomenon is observed in numerous materials [49,50]. Figure 6 illustrates the evolution of the PL spectra at 17 K for various power excitation densities.…”
Section: Resultsmentioning
confidence: 98%
“…Among other semiconductors, the intrinsic binary InSb possesses the highest electron mobility (∼7.8 × 10 4 cm 2 /V•s), higher breakdown field (∼10 3 V/cm), high saturated electron drift velocity (∼5 × 10 7 cm/s), small effective mass (m * e ∼0.013 m o ), lowest energy band gap E g ∼0.18 eV (at 300 K), and ballistic length up to ∼0.7 μm (at 300 K). e InSb material can be used as a lattice-matched substrate for epitaxial growth of CdTe [34] and other relevant heterostructures and superlattices [35]. e InSb-based ternary as well as quaternary alloys are equally valuable for realizing midwavelength infrared detectors [36][37][38][39].…”
Section: Introductionmentioning
confidence: 99%