TY - JOUR
T1 - Raman scattering study of GeTe and Ge2Sb2Te5 phase-change materials
AU - Andrikopoulos, K. S.
AU - Yannopoulos, S. N.
AU - Kolobov, A. V.
AU - Fons, P.
AU - Tominaga, J.
N1 - Funding Information:
The Greek side acknowledges financial support from the General Secretariat for Research and Technology—Hellas in the framework of the bilateral project GR-CZ (2005–2007).
PY - 2007/5
Y1 - 2007/5
N2 - Structural details of the amorphous binary GeTe and ternary Ge2Sb2Te5 (GST) phase-change materials are investigated with the aid of Raman scattering. In the case of the a-GeTe, a plethora of Raman bands have been recorded and assigned on the basis of a network structure consisting of corner- and edge-sharing tetrahedra of the type GeTe4-nGen (n=0, 1, 2, 3, 4). Significant temperature-induced structural changes take place in this material even at temperatures well below the crystallization temperature. These changes tend to organize the local structure, in particular the coordination number of Ge atoms, so as to facilitate the amorphous-to-crystal transformation. The much simpler Raman spectrum of GST, characterized by one vibrational band, is accounted for by the dominance of the Sb2T3 component in Raman scattering; reasons about this explanation, as well as for the lack of any Te-Te bonds are briefly described.
AB - Structural details of the amorphous binary GeTe and ternary Ge2Sb2Te5 (GST) phase-change materials are investigated with the aid of Raman scattering. In the case of the a-GeTe, a plethora of Raman bands have been recorded and assigned on the basis of a network structure consisting of corner- and edge-sharing tetrahedra of the type GeTe4-nGen (n=0, 1, 2, 3, 4). Significant temperature-induced structural changes take place in this material even at temperatures well below the crystallization temperature. These changes tend to organize the local structure, in particular the coordination number of Ge atoms, so as to facilitate the amorphous-to-crystal transformation. The much simpler Raman spectrum of GST, characterized by one vibrational band, is accounted for by the dominance of the Sb2T3 component in Raman scattering; reasons about this explanation, as well as for the lack of any Te-Te bonds are briefly described.
KW - A. Amorphous materials
KW - A. Chalcogenides
KW - C. Raman spectroscopy
KW - D. Phase transitions
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U2 - 10.1016/j.jpcs.2007.02.027
DO - 10.1016/j.jpcs.2007.02.027
M3 - Article
AN - SCOPUS:34250180554
SN - 0022-3697
VL - 68
SP - 1074
EP - 1078
JO - Journal of Physics and Chemistry of Solids
JF - Journal of Physics and Chemistry of Solids
IS - 5-6
ER -