1972
DOI: 10.1002/pssa.2210110206
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Study of the mechanism of radiative recombination in vitreous and monocrystalline arsenic selenide

Abstract: The temperature dependences of the intensity and spectral characteristics of the steady‐state photoluminescence in vitreous and monocrystalline As2Se3 are studied over the range 4 to 150 °K. The interpretation of the experimental data is based on the idea about the existence of a band of deep levels in the gap of both the glass and the crystal which are responsible for the radiation. It is concluded that the disorder leads to the disappearance of the centres which are capable of taking part in the nonradiative… Show more

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Cited by 30 publications
(4 citation statements)
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“…The broad peak at 2.7 eV contributes to the blue light emission. The above features in the PL spectra are true for all temperatures from 20 to 292 K. Similar temperature-insensitive peak position and linewidth were observed in the PL spectra of chalcogenide glasses [5]. The luminescence intensity, however, strongly depends on temperature as shown in Fig.…”
Section: 100 95supporting
confidence: 66%
See 1 more Smart Citation
“…The broad peak at 2.7 eV contributes to the blue light emission. The above features in the PL spectra are true for all temperatures from 20 to 292 K. Similar temperature-insensitive peak position and linewidth were observed in the PL spectra of chalcogenide glasses [5]. The luminescence intensity, however, strongly depends on temperature as shown in Fig.…”
Section: 100 95supporting
confidence: 66%
“…(2) to the model in Fig. 6, the transition rates from the radiative to the nonradiative recombination centers via tunneling, P4 and P 5 , are given by P 4 = p4.exp(T/T 4 3 ) (5) and…”
Section: 100 95mentioning
confidence: 99%
“…In the first place, these are reversible photostructural conversions leading to changes in many properties of CGS. It was shown in classical works [3,4] that photoluminescence spectra of As 2 Se 3 , As 2 S 3 , GeSe 2 single crystals, and appropriate CGS exhibit a single photoluminescence band (PL) with hν ≤ E q /2 (E q . is the width of the forbidden band), quantum efficiency of η = 0.2 -0.5, and large Stokes shift, W S ≥ 1 eV.…”
Section: Introductionmentioning
confidence: 99%
“…Then (a possible) energy dependence of the localization radius y = y ( E ) converts into a non-exponential frequency dependence.l) l) The reason for this behaviour is obvious: I n the uncorrelated case all possible relative distances R,,(20) are realized with equal probability. Then the major contribution to the double sum (9) (or multiple integral (18)) is due to pairs of initial and final states where exp (--yR,,) = 1, i.e.…”
mentioning
confidence: 99%