Archives of Metallurgy and Materials (Jun 2015)

Photoinduced Optical Properties Of Tl1−xIn1−xSixSe2 Single Crystals

  • Myronchuk G.L.,
  • Zamurueva O.V.,
  • Oźga K.,
  • Szota M.,
  • El-Naggar A.M.,
  • Alzayed N.S.,
  • Piskach L.V.,
  • Parasyuk O.V.,
  • Albassam A.A.,
  • Fedorchuk A.O.,
  • Kityk I.V.

DOI
https://doi.org/10.1515/amm-2015-0258
Journal volume & issue
Vol. 60, no. 2
pp. 1051 – 1055

Abstract

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The influence of temperature on electroconductivity and photoinduced changes of the absorption at 0.15 eV under influence of the second harmonic generation of CO2 laser for the two type of single crystals were investigated. The single crystals Tl1−xIn1−xSixSe2 (x=0.1 and 0.2) have been grown by the two-zone Bridgaman-Stockbarger method. The temperature studies of electroconductivity were done in cryostat with thermoregulation in the temperature 77 - 300 K, with stabilization ±0.1 K. Photoinduced treatment of the investigated single crystals were performed using the 180 ns pulses second harmonic generation of the CO2 laser operating at 5.3 μm. Experimental studies have shown that for the Tl1−xIn1−xSixSe2 single crystals with decreasing temperature from 300 up to 240 K and from 315 up to 270 K the conductivity is realized by thermally excited impurities with activation energies equal to about 0.24 eV and 0.22 eV for x= 0.1 and 0.2, respectively. Photoinduced absorption achieves its maximum at a power density below 100 mJ/cm2. Has been shown that the samples with x=0.2 demonstrated higher changes of the photoinduced absorption with respect to the x=0.1. With further decreasing temperature is observed monotonic decrease in the activation energy of conductivity. The origin of these effects is caused by the excitations of both the electronic as well as phonon subsystem. At some power densities the anharmonic excitations become dominant and as a consequence the photoinduced absorption dependence is saturated what were observed. Additionally, we were evaluated at given temperature the average jump length of R for localized states near Fermi level.

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