2011
DOI: 10.1103/physrevb.83.092102
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Pressure-induced phase transition of Bi2Te3to a bcc structure

Abstract: The pressure-induced phase transition of bismuth telluride, Bi 2 Te 3 , has been studied by synchrotron x-ray diffraction measurements at room temperature using a diamond-anvil cell (DAC) with loading pressures up to 29.8 GPa. We found a high-pressure body-centered cubic (bcc) phase in Bi 2 Te 3 at 25.2 GPa, which is denoted as phase IV, and this phase apperars above 14.5 GPa.Upon releasing the pressure from 29.8 GPa, the diffraction pattern changes with pressure hysteresis. The original rhombohedral phase is … Show more

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Cited by 83 publications
(65 citation statements)
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“…The phase transition routines are in good accordance with the recent reports on the corresponding bulk Bi 2 Te 3 and Sb 2 Te 3 materials. 33,34,38 The ambient peak of (015) crystal plane centered at 2θ of ∼11.02°r emained up to 9.2 GPa and even existed as the pressure was further increased to 10.9 GPa, which is clearly marked with the arrow. However, new Bragg peaks denoted by open asterisks emerged as soon as the loading pressure reached 9.2 GPa, signifying the onset of initial structural phase transition to a monoclinic structured Bi 2 Te 3 (phase II).…”
Section: ■ Experimental Sectionmentioning
confidence: 93%
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“…The phase transition routines are in good accordance with the recent reports on the corresponding bulk Bi 2 Te 3 and Sb 2 Te 3 materials. 33,34,38 The ambient peak of (015) crystal plane centered at 2θ of ∼11.02°r emained up to 9.2 GPa and even existed as the pressure was further increased to 10.9 GPa, which is clearly marked with the arrow. However, new Bragg peaks denoted by open asterisks emerged as soon as the loading pressure reached 9.2 GPa, signifying the onset of initial structural phase transition to a monoclinic structured Bi 2 Te 3 (phase II).…”
Section: ■ Experimental Sectionmentioning
confidence: 93%
“…26,27 Despite the special interest in it, response of Bi 2 Te 3 to high pressure has been yet rarely explored. 28−32 Recently, Bi−Te subtutional nonmetallic alloy has been successfully achieved at pressure above 25 GPa, 33,34 making high pressure a highly attractive route to synthesize novel alloys. Otherwise, best endeavoring to satisfy energy conservation remains a major concern to date, hence encouraging us to seek how to lower the applied pressure for the preparation of nonmetallic element alloys.…”
Section: ■ Introductionmentioning
confidence: 99%
“…12 The study of physical properties in these materials under compression is receiving increasing attention especially due to continuous experimental and theoretical developments. [13][14][15][16][17][18][19][20][21][22] The high-pressure phases II, III, and IV of Bi 2 Te 3 were recognized by x-ray diffraction experiments with the additional help from the particle swarm optimization algorithm. [13][14][15] The same type of phases was observed in Bi 2 Se 3 and Sb 2 Te 3 by the experiment group of Vilaplana et al 16,17 Here, the phase transition from the α phase I to the β phase II was between the rhombohedral R3m crystal structure to the monoclinic C2/m structure at 10 GPa for Bi 2 Se 3 , 7.4 GPa for Bi 2 Te 3 , and 7.7 GPa for Sb 2 Te 3 .…”
Section: Introductionmentioning
confidence: 99%
“…The application of pressure has recently been reported to turn the topological insulator Bi 2 Te 3 into a superconducting state18. Isostructural to Bi 2 Te 3 and Bi 2 Se 3 19202122232425, Sb 2 Te 3 is another well-studied three-dimensional topological insulator. In this study, we report the discovery of superconductivity in Sb 2 Te 3 single crystals induced via pressure.…”
mentioning
confidence: 99%