1985
DOI: 10.1016/0375-9601(85)90521-3
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Plasma phase transition in hydrogen

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Cited by 123 publications
(50 citation statements)
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“…The occurrence of metallization induced by pressure was discussed by Wigner and Huntington, 1935 for atomic hydrogen at T=0K, by Landau and Zeldovich, 1943 for liquid mercury as a first order phase transition, and by Norman and Starostin, 1970 for a dense atomic plasma. In high pressure fluid hydrogen, molecular dissociation and ionization was discussed by Ebeling et al (Ebeling and Richert, 1985;Ebeling and W., 1985) and later by other authors (Beule et al, 1999;Edwards et al, 2010;Fortov et al, 2003a;Kitamura and Ichimaru, 1998;Marley and Hubbard, 1988;Redmer and Holst, 2010;Saumon and Chabrier, 1989, 1992 at several levels of sophistication in the framework of chemical models. These models exhibit a clear first-order liquid-liquid transition (LLT) that persists for temperatures well above 10,000 K. However, approaches with separate free energy functionals in different regions of phase space have great difficulty in having a continuous crossover from one behavior to another.…”
Section: Liquid-liquid Phase Transitionmentioning
confidence: 99%
“…The occurrence of metallization induced by pressure was discussed by Wigner and Huntington, 1935 for atomic hydrogen at T=0K, by Landau and Zeldovich, 1943 for liquid mercury as a first order phase transition, and by Norman and Starostin, 1970 for a dense atomic plasma. In high pressure fluid hydrogen, molecular dissociation and ionization was discussed by Ebeling et al (Ebeling and Richert, 1985;Ebeling and W., 1985) and later by other authors (Beule et al, 1999;Edwards et al, 2010;Fortov et al, 2003a;Kitamura and Ichimaru, 1998;Marley and Hubbard, 1988;Redmer and Holst, 2010;Saumon and Chabrier, 1989, 1992 at several levels of sophistication in the framework of chemical models. These models exhibit a clear first-order liquid-liquid transition (LLT) that persists for temperatures well above 10,000 K. However, approaches with separate free energy functionals in different regions of phase space have great difficulty in having a continuous crossover from one behavior to another.…”
Section: Liquid-liquid Phase Transitionmentioning
confidence: 99%
“…Going to bigger system sizes N P = 64 and using FP nodes also shows a shift towards lower densities. [1,2] with PIMC simulation (VDM nodes, τ −1 = 2 · 10 6 K) and several theoretical approaches: SESAME model by Kerley [3] (thin solid line), linear mixing model by Ross (dashed line) [4], DFT-MD by Lenosky et al [8] (dash-dotted line), Padé approximation in the chemical picture (PACH) by Ebeling et al [11] (dotted line), and the work by Saumon et al [10] (thin dash-dotted line).…”
Section: Shock Hugoniotmentioning
confidence: 99%
“…Further there are models that minimize an approximate free energy function constructed from known theoretical limits with respect to the chemical composition, which work very well in certain regimes. The most widely used include [10,11,4].…”
mentioning
confidence: 99%
“…https://doi.org/10.1017/S0252921100026415 same critical point, at T c = 16500 K, P c = 0.228 Mbar and p c = 0.13 gem -3 . In the first model (Ebeling and Richert 1985a), atoms and molecules interact through hard-sphere potentials with fixed diameters, plus a Van-der-Waals correction. Molecules are approximated as two atoms in the hard-sphere free energy.…”
Section: Other Modelsmentioning
confidence: 99%