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High-pressure phase transitions in Zn1-xMxSe (M=Cd, Fe, and Mn)

dc.citation.epage19en_US
dc.citation.issue1en_US
dc.citation.spage16en_US
dc.citation.volume58en_US
dc.citation.woscount16en_US
dc.contributor.authorLin, CMen_US
dc.contributor.authorChuu, DSen_US
dc.contributor.authorXu, JAen_US
dc.contributor.authorHuang, Een_US
dc.contributor.authorChou, WCen_US
dc.contributor.authorHu, JZen_US
dc.contributor.authorPei, JHen_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.date.accessioned2019-04-03T06:35:48Z
dc.date.available2019-04-03T06:35:48Z
dc.date.issued1998-07-01en_US
dc.description.abstractEnergy-dispersive x-ray diffraction was employed to study pressure-induced phase transitions in Zn0.84Fe0.16Se, Zn0.9Cd0.1Se, and Zn0.76Mn0.24Se crystals up to 21.0, 23.3, and 24.3 GPa, respectively. Our result shows that the B3 to B1 structure transitions for these crystals occurred at 1 1.4 +/- 0.5, 9.5 +/- 0.3, and 9.6 +/- 0.5 GPa, respectively. Compared to the phase-transition pressure (P-t) of ZnSe (14.4 GPa), a reduction of about 3-5 GPa is exhibited in these ternary compounds. This reduction in phase-transition pressure Delta P-t in the ternary compounds suggests that the fractional volume change, (Delta V/V-o), of the B3-B1 phase admixture might be the source of this reduction. Our results indicate that P-t (with respect to the phase transition pressure 14.4 GPa of ZnSe) is related to the fractional volume change (Delta V/V-o) by the expression P-t = [14.4003 + 0.1568 (Delta V/V-o)-0.0281(Delta V/V-o)(2)] GPa. [S0163-1829(98)05426-5].en_US
dc.identifier.doi10.1103/PhysRevB.58.16en_US
dc.identifier.issn1098-0121en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.58.16en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/32517
dc.identifier.wosnumberWOS:000074643200005en_US
dc.language.isoen_USen_US
dc.titleHigh-pressure phase transitions in Zn1-xMxSe (M=Cd, Fe, and Mn)en_US
dc.typeArticleen_US

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