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High-temperature structural phase transitions of GexS1-x alloys studied by raman spectroscopy

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dc.contributor.author Kotsalas, IP en
dc.contributor.author Raptis, C en
dc.date.accessioned 2014-03-01T01:16:37Z
dc.date.available 2014-03-01T01:16:37Z
dc.date.issued 2001 en
dc.identifier.issn 0163-1829 en
dc.identifier.uri https://dspace.lib.ntua.gr/xmlui/handle/123456789/14122
dc.subject High Temperature en
dc.subject Raman Spectroscopy en
dc.subject Structural Phase Transition en
dc.subject.classification Physics, Condensed Matter en
dc.subject.other alloy en
dc.subject.other germanium en
dc.subject.other sulfur en
dc.subject.other article en
dc.subject.other chemical structure en
dc.subject.other cooling en
dc.subject.other crystallization en
dc.subject.other high temperature procedures en
dc.subject.other melting point en
dc.subject.other phase transition en
dc.subject.other Raman spectrometry en
dc.subject.other stoichiometry en
dc.title High-temperature structural phase transitions of GexS1-x alloys studied by raman spectroscopy en
heal.type journalArticle en
heal.identifier.primary 10.1103/PhysRevB.64.125210 en
heal.identifier.secondary http://dx.doi.org/10.1103/PhysRevB.64.125210 en
heal.identifier.secondary 125210 en
heal.language English en
heal.publicationDate 2001 en
heal.abstract A high-temperature Raman study of GexS1-x alloys is reported up to a temperature close to the melting point, including both Ge-rich (x=0.35) and S-rich (x=0.20,0.30) glasses, as well as the compound glass (g-GeS; x=1/3). The variation in the Raman spectra indicates that above certain temperatures g-GeS2 gradually crystallizes, first to the three-dimensional (3D) phase and then to the layered two-dimensional (2D) phase, with the latter being maintained up to melting point and upon subsequent cooling to room temperature. There is evidence that the controversial Al companion band of g-GeS2 evolves to a counterpart band of the 2D crystalline phase, implying that this band is due to symmetric stretch vibrations of S atoms in bridges of edge-sharing Ge(S-1/2)(4) tetrahedra, in agreement with a previous prediction. Similar two step irreversible crystallization to the 3D and 2D phases of GeS2 have been observed above T-g for the moderately rich in Ge (x=0.35) or in S (x=0.30) GexS1-x glasses, but at lower thresholds of crystallization temperature. In the strongly enriched in S (x=0.20) glass, though, crystallization takes place only to the 3D phase of GeS2, a process which is reversible after cooling the alloy to room temperature, i.e., the material returns to its initial amorphous phase. This reversible crystallization is explained in terms of the three-dimensional network of S-rich GexS1-x glasses which evolves only to the respective 3D crystalline phase lattice at high temperatures. It is pointed out that all GexS1-x glasses studied undergo a first-step transition to the 3D crystalline phase, which shows that the network of these glasses is, by large, three dimensional. en
heal.publisher AMERICAN PHYSICAL SOC en
heal.journalName Physical Review B - Condensed Matter and Materials Physics en
dc.identifier.doi 10.1103/PhysRevB.64.125210 en
dc.identifier.isi ISI:000171244400059 en
dc.identifier.volume 64 en
dc.identifier.issue 12 en
dc.identifier.spage 1252101 en
dc.identifier.epage 1252108 en


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