1984
DOI: 10.1016/0375-9601(84)90757-6
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Phase transitions in alkaline earth metals under pressure

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Cited by 152 publications
(128 citation statements)
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“…Nevertheless, the values for the equilibrium volume V 0 , bulk modulus B 0 and its derivative BЈ 0 , which from our calculation are 42.19 Å 3 , 17.46 GPa, and 3.14, respectively, are in close agreement with the corresponding experimental parameters of the equations of state (20). Calculated volume collapse ⌬V/V of 1% and 7% at the cF4 3 cI2 and cI2 3 cP1 phase transitions, respectively, are also in good agreement with the experiment (14).…”
Section: Resultssupporting
confidence: 75%
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“…Nevertheless, the values for the equilibrium volume V 0 , bulk modulus B 0 and its derivative BЈ 0 , which from our calculation are 42.19 Å 3 , 17.46 GPa, and 3.14, respectively, are in close agreement with the corresponding experimental parameters of the equations of state (20). Calculated volume collapse ⌬V/V of 1% and 7% at the cF4 3 cI2 and cI2 3 cP1 phase transitions, respectively, are also in good agreement with the experiment (14).…”
Section: Resultssupporting
confidence: 75%
“…Ca shows an interesting and unique phase transition sequence from a closed, packed structure at ambient pressure to an open one at high pressures, namely, a face-centered cubic cF4 to a body-centered cubic cI2 transition at Ϸ19.5 GPa (13,14), and a cI2 to a simple cubic cP1 phase transition at 32 GPa (14). This remarkable transition sequence was found to occur because of the same s-band to d-band electron transfer, and that at high pressures the valence band acquires a complete d-like character (15).…”
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confidence: 99%
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“…The series of surprising high-pressure phase transitions (6)(7)(8)(9) that change the elemental Ca from an ordinary metal to the highest known T c (>25 K) elemental superconductor (8) has emerged as a central topic as demonstrated in many concurrent investigations (10-17) but also presented a seemingly irreconcilable gap between theory and experiment. X-ray diffraction (XRD) at 300 K indicates that Ca transforms from its ambient condition fcc structure Ca-I to bodycentered cubic (bcc) Ca-II at 20 GPa and then to simple-cubic (sc) Ca-III at 32 GPa (7,9,18). At higher pressures, Ca-III undergoes two additional transformations, to Ca-IV and V at 119 and 143 GPa, respectively (7,9,18).…”
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confidence: 99%
“…The critical role of the pressure-induced s to d band electron transfer on the structural stability and physical properties, such as superconductivity, of metals has been studied extensively over the years [1][2][3][4]. High pressure structural sequences in 3 rd period metals have also been elucidated when taking into account the lowering and filling under compression of the initially vacant d-band [5,6].…”
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confidence: 99%