2019
DOI: 10.1134/s1063783419010281
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Absolute Instability of FCC Lattice of Rare-Gas Crystals under Pressure

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Cited by 6 publications
(2 citation statements)
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“…140 We showed recently that the fcc phase is stabilized by phonon dispersion at 0 K. 34 As phonon contributions play a lesser role at increased pressures, one can speculate that three-body and higher body contributions must be responsible for the phase change to hcp at higher pressures. 141 From a theoretical point of view, to simulate a phase transition with such small enthalpy differences remains a major challenge. If experimental data were fitted to many-body potentials, based for example on the embedded atom model, one can obtain more accurate results.…”
Section: ■ Methodsmentioning
confidence: 99%
“…140 We showed recently that the fcc phase is stabilized by phonon dispersion at 0 K. 34 As phonon contributions play a lesser role at increased pressures, one can speculate that three-body and higher body contributions must be responsible for the phase change to hcp at higher pressures. 141 From a theoretical point of view, to simulate a phase transition with such small enthalpy differences remains a major challenge. If experimental data were fitted to many-body potentials, based for example on the embedded atom model, one can obtain more accurate results.…”
Section: ■ Methodsmentioning
confidence: 99%
“…136 We showed recently that the fcc phase is stabilized by phonon dispersion at 0 K. 32 As phonon contributions play a lesser role at increased pressures, one can speculate that threeand higher body contributions must be responsible for the phase change to hcp at higher pressures. 137 From a theoretical point of view, to simulate a phase transition with such small enthalpy differences remains a major challenge. If experimental data fitted to many-body potentials, based for example on the embedded atom model, one can obtain more accurate results.…”
Section: The Equation Of State For Solid Heliummentioning
confidence: 99%