2015
DOI: 10.1063/1.4929257
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Structural analysis of quaternary Se85−xSb10In5Agx bulk glassy alloys

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Cited by 2 publications
(2 citation statements)
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“…One another weak peak at ~ 210 cm -1 can be ascribed from either Se-Se chain bond or asymmetrical stretching of pyramidal SbSe3 mode [21]. The broad band at 188 cm -1 can be assigned to heteropolar Sb˗Se bond vibrations in Sb(Se1/2)3 pyramidal structural units [22]. With the increase in indium content, the intensity of two domi-nant peaks at 188 and 250 cm -1 decreases and fades away for x  20, 25 and favours the nucleation of new band at 212 cm -1 which is due to the vibrations of In and Se atoms.…”
Section: Raman Analysismentioning
confidence: 99%
“…One another weak peak at ~ 210 cm -1 can be ascribed from either Se-Se chain bond or asymmetrical stretching of pyramidal SbSe3 mode [21]. The broad band at 188 cm -1 can be assigned to heteropolar Sb˗Se bond vibrations in Sb(Se1/2)3 pyramidal structural units [22]. With the increase in indium content, the intensity of two domi-nant peaks at 188 and 250 cm -1 decreases and fades away for x  20, 25 and favours the nucleation of new band at 212 cm -1 which is due to the vibrations of In and Se atoms.…”
Section: Raman Analysismentioning
confidence: 99%
“…The presence of any weak band at 138-145 cm −1 is often associated to Se-Se banding vibration mode [31]. For this reason, peak at 140.23 ± 0.65 cm −1 can be attributed and polymeric Se chains (as in trigonal Se with helicoidal chains), respectively [32][33][34][35][36]. For x = 0.08 the peak at 177.22 ± 1.73 cm −1 shifts to 182.69 ± 0.76 cm −1 and for x = 0.12 it shifts to 188.91 ± 1.20 cm −1 whereas peak at 201.88 ± 1.21 cm −1 shifts to 211.46 ± 0.24 cm −1 for x = 0.08 and to 212.57 ± 0.32 cm −1 for x = 0.12.…”
Section: Raman Analysismentioning
confidence: 99%