1970
DOI: 10.1016/0038-1098(70)90619-8
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Soft phonon mode and ferroelectricity in GeTe

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Cited by 182 publications
(139 citation statements)
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“…The previous Raman spectroscopy studies on bulk single crystal α-GeTe showed both E and A 1 modes at 93 and 127 cm −1 at room temperature, where the later one found to be as soft optical phonon mode. 21 In the present work, we observe the both E and A 1 modes at 88.4 and 125.7 cm −1 at 298 K with 10 µm crystal size and these results are closer to those reported earlier on single crystal of α-GeTe. However, the recent experimental study on bulk polycrystalline α-GeTe specimen reveals that the Raman modes of E and A 1 occur at 95 and 125 cm −1 along with additional bands with lesser intensity at high frequencies.…”
Section: Resultssupporting
confidence: 92%
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“…The previous Raman spectroscopy studies on bulk single crystal α-GeTe showed both E and A 1 modes at 93 and 127 cm −1 at room temperature, where the later one found to be as soft optical phonon mode. 21 In the present work, we observe the both E and A 1 modes at 88.4 and 125.7 cm −1 at 298 K with 10 µm crystal size and these results are closer to those reported earlier on single crystal of α-GeTe. However, the recent experimental study on bulk polycrystalline α-GeTe specimen reveals that the Raman modes of E and A 1 occur at 95 and 125 cm −1 along with additional bands with lesser intensity at high frequencies.…”
Section: Resultssupporting
confidence: 92%
“…However, the recent experimental study on bulk polycrystalline α-GeTe specimen reveals that the Raman modes of E and A 1 occur at 95 and 125 cm −1 along with additional bands with lesser intensity at high frequencies. 22 On the basis of ab initio results [17][18][19][20] and earlier Raman spectroscopy observations, 21,22 we confirm that the observed vibrational modes in 10µm crystal size are intrinsic part of bulk α-GeTe structure. Furthermore, the decrease in crystal size leads to downshift of phonon modes in addition to the peak broadening of the Raman spectra as shown in inset of Figure 3.…”
Section: Resultssupporting
confidence: 82%
“…In other words, the material exhibits a displacive phase transition, similar to that of perovskite ferroelectrics, with the dipole moment in the low-temperature phase stemming from the relative shift of Ge and Te sublattices. 10 Raman scattering studies showed some mode softening, 11 which provided indirect support of the proposed structural change. This description of the phase transition has been recently challenged by extended X-ray absorption fine structure (EXAFS) 12 and total scattering studies.…”
mentioning
confidence: 84%
“…The authors concluded that the ferroelectricto-paraelectric transition results from an order-disorder transition, where the structure remains rhombohedrally distorted locally but the distortions change from coherent at low temperatures to stochastic at higher temperatures. [9][10][11] In the latter case, the average structure becomes cubic. This discrepancy between the Bragg diffraction and the EXAFS/total scattering results is not unknown and has also been reported for other materials.…”
mentioning
confidence: 99%
“…GeTe might make a promising ferroelectric were it not for large concentrations of free carriers arising from Ge vacancies and a Fermi energy lying within the valence band. [19][20][21] Again, the GeTe structure is a consequence of s-p hybridization and lone pairs on both Ge and Te. 22 SnTe also forms the rhombohedral A7 structure below ∼16 K, 23,24 while all other IV-VI compounds form the rocksalt or GeS structures at room temperature.…”
Section: Fig 1 (Color Online)mentioning
confidence: 99%