2005
DOI: 10.1016/j.ssc.2004.11.035
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Hexagonal to cubic phase transition in YH3 under high pressure

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Cited by 52 publications
(50 citation statements)
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“…Once the C2 / m structure completely changes to fcc at 38 GPa, the band gap closes completely and YH 3 becomes metallic. The pressure-dependent insulating properties of the C2 / m structure agree well with the experimental observation [4][5][6][7] for the intermediate phase in this pressure range.…”
supporting
confidence: 86%
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“…Once the C2 / m structure completely changes to fcc at 38 GPa, the band gap closes completely and YH 3 becomes metallic. The pressure-dependent insulating properties of the C2 / m structure agree well with the experimental observation [4][5][6][7] for the intermediate phase in this pressure range.…”
supporting
confidence: 86%
“…A series of studies have characterized the highpressure phase transitions for YH 3 up to 40 GPa. [2][3][4][5][6][7][8] At ambient pressure, YH 3 forms a distorted hcp form identified with space group P3c1 by neutron diffraction. [9][10][11] There are two other suggested possible structures 12,13 that are almost energetically degenerate but not in agreement with recent neutron-diffraction data.…”
mentioning
confidence: 99%
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“…1,2) Recently, an abrupt closure of the optical gap at 23 GPa was reported by Ohmura et al; the transmission intensity became zero in the infrared region. 3) They claimed that this might indicate that an insulator-tometal transition was induced by the overlap of the electron orbitals of neighboring hydrogen atoms.…”
Section: Introductionmentioning
confidence: 88%