Abstract:Despite the extensive and systematic studies of pressure-induced phase transitions in sesqui-chalcogenides, several puzzles still remain to be solved. Here, the complicated phase transitions, amorphization, and alloying behaviors of the...
“…81 Usually, about ten modes are clearly distinguishable. 20,21,26 The Raman spectrum of L-Sb 2 S 3 at 873 K appears to be reminiscent of its glassy counterpart, Fig. 4(d), except for a strong S-S stretching at 490 cm À1 .…”
Section: Nanocrystalline Sb 2 Smentioning
confidence: 94%
“…The crystal structure of Sb 2 S 3 has been extensively studied both under ambient conditions [16][17][18] and under high pressure. [19][20][21][22][23][24][25][26] Nevertheless, the atomic structure of vitreous and liquid antimony sesquisulfide is largely unknown except for classical X-ray diffraction studies of glassy Sb 2 S 3 reported forty years ago and suffering from a limited accessible Q-range and insufficient r-space resolution. [27][28][29] In the case of PCM applications, [30][31][32] special attention should be paid to the origin of a high optical and electric contrast between the SET (crystalline) and RESET (amorphous) logic states since antimony sesquisulfide differs considerably from the benchmark telluride PCM (GeTe-Sb 2 Te 3 , GST, or doped Sb 2 Te) in both chemical bonding and local antimony environments.…”
High optical and electric contrast between the SET (crystalline) and RESET (amorphous) logic states is related to the different short and intermediate range order in orthorhombic and vitreous Sb2S3.
“…81 Usually, about ten modes are clearly distinguishable. 20,21,26 The Raman spectrum of L-Sb 2 S 3 at 873 K appears to be reminiscent of its glassy counterpart, Fig. 4(d), except for a strong S-S stretching at 490 cm À1 .…”
Section: Nanocrystalline Sb 2 Smentioning
confidence: 94%
“…The crystal structure of Sb 2 S 3 has been extensively studied both under ambient conditions [16][17][18] and under high pressure. [19][20][21][22][23][24][25][26] Nevertheless, the atomic structure of vitreous and liquid antimony sesquisulfide is largely unknown except for classical X-ray diffraction studies of glassy Sb 2 S 3 reported forty years ago and suffering from a limited accessible Q-range and insufficient r-space resolution. [27][28][29] In the case of PCM applications, [30][31][32] special attention should be paid to the origin of a high optical and electric contrast between the SET (crystalline) and RESET (amorphous) logic states since antimony sesquisulfide differs considerably from the benchmark telluride PCM (GeTe-Sb 2 Te 3 , GST, or doped Sb 2 Te) in both chemical bonding and local antimony environments.…”
High optical and electric contrast between the SET (crystalline) and RESET (amorphous) logic states is related to the different short and intermediate range order in orthorhombic and vitreous Sb2S3.
“…53,67 The minor peaks around 240 and 330 cm −1 can be ascribed to the vibrations of B 2g and B 3g assigned modes. 53,67…”
Section: Resultsmentioning
confidence: 98%
“…The weak peaks around 100 cm −1 and major peaks near 70 cm −1 can be attributed to the A g assigned modes. 53,67 The peak around 170 cm −1 can be assigned to the B 1g assigned modes. 53,67 The minor peaks around 240 and 330 cm −1 can be ascribed to the vibrations of B 2g and B 3g assigned modes.…”
Section: Resultsmentioning
confidence: 99%
“…53,67 The peak around 170 cm −1 can be assigned to the B 1g assigned modes. 53,67 The minor peaks around 240 and 330 cm −1 can be ascribed to the vibrations of B 2g and B 3g assigned modes. 53,67…”
By performing nonadiabatic molecular dynamics combined with ab initio time-domain density functional theory, we have explored the effects of charge density of sulfur vacancy on the charge trapping and recombination...
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