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Volumn 65, Issue 5, 2002, Pages 1-4

Melting curve equations at high pressure

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EID: 85038276148     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.65.052102     Document Type: Article
Times cited : (14)

References (58)
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    • The Simon-Glatzel equation is commonly used in the three-parameter form (formula presented) and even in the four-parameter form (formula presented)
    • The Simon-Glatzel equation is commonly used in the three-parameter form (formula presented) and even in the four-parameter form (formula presented) [K. Crawford and W. B. Daniels, J. Chem. Phys. 55, 565 (1971)].
    • (1971) J. Chem. Phys. , vol.55 , pp. 565
    • Crawford, K.1    Daniels, W.B.2
  • 41
    • 0008240813 scopus 로고
    • Dass has used the linear dependence for the Grüneisen parameter γ and isothermal bulk modulus (formula presented) on pressure and calculated the melting curve maximum for alkali metals
    • Dass has used the linear dependence for the Grüneisen parameter γ and isothermal bulk modulus (formula presented) on pressure and calculated the melting curve maximum for alkali metals [N. Dass, Phys. Rev. B 52, 3023 (1995)].
    • (1995) Phys. Rev. B , vol.52 , pp. 3023
    • Dass, N.1
  • 43
    • 85038306664 scopus 로고
    • High Pressure Phase Transitions: A Handbook, edited by E. Yu. Tonkov (Gordon and Breach, Philadelphia
    • High Pressure Phase Transitions: A Handbook, edited by E. Yu. Tonkov (Gordon and Breach, Philadelphia, 1992), Vols. 1 and 2.
    • (1992) , vol.1-2
  • 49
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    • R. Boehler, Physica A 139/140, 233 (1986).
    • (1986) Physica A , vol.139-140 , pp. 233
    • Boehler, R.1
  • 53
    • 0008202990 scopus 로고
    • Theory predicts that metallic hydrogen will remain a fluid at all pressures In this case, we have a unique situation: the melting curve is simultaneously the distinct curve between molecular and atomic and the distinct curve between nonmetallic and metallic hydrogen at high pressure
    • Theory predicts that metallic hydrogen will remain a fluid at all pressures [A. H. MacDonald and C. P. Burgess, Phys. Rev. B 26, 2849 (1982)]. In this case, we have a unique situation: the melting curve is simultaneously the distinct curve between molecular and atomic and the distinct curve between nonmetallic and metallic hydrogen at high pressure.
    • (1982) Phys. Rev. B , vol.26 , pp. 2849
    • MacDonald, A.H.1    Burgess, C.P.2
  • 55
    • 4243549489 scopus 로고
    • More likely the broad melting curve minimum of Ce comprises the melting-curve segments of α, (formula presented) and tetragonal phases
    • More likely the broad melting curve minimum of Ce comprises the melting-curve segments of α, (formula presented) and tetragonal phases [S. Endo and N. Fujioka, Phys. Lett. 70A, 475 (1979).
    • (1979) Phys. Lett. , vol.70 A , pp. 475
    • Endo, S.1    Fujioka, N.2
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    • 9, 31 (1970).
    • (1970) , vol.9 , pp. 31


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.