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Volumn 130, Issue 12, 2009, Pages

Polyamorphism in tin tetraiodide

Author keywords

[No Author keywords available]

Indexed keywords

LIQUIDS; PHASE DIAGRAMS; PHOSPHORUS; TIN; TITANIUM COMPOUNDS;

EID: 63649090582     PISSN: 00219606     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.3109691     Document Type: Article
Times cited : (18)

References (27)
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    • Glosli, J.N.1    Ree, F.H.2
  • 6
    • 28844445080 scopus 로고    scopus 로고
    • 0031-9007 10.1103/PhysRevLett.95.185701.
    • X. Wang, S. Scandolo, and R. Car, Phys. Rev. Lett. 0031-9007 10.1103/PhysRevLett.95.185701 95, 185701 (2005).
    • (2005) Phys. Rev. Lett. , vol.95 , pp. 185701
    • Wang, X.1    Scandolo, S.2    Car, R.3
  • 10
    • 7444237150 scopus 로고    scopus 로고
    • 0036-8075 10.1126/science.1103073.
    • R. Kurita and H. Tanaka, Science 0036-8075 10.1126/science.1103073 306, 845 (2004).
    • (2004) Science , vol.306 , pp. 845
    • Kurita, R.1    Tanaka, H.2
  • 12
    • 0000790865 scopus 로고
    • 0022-3719 10.1088/0022-3719/18/4/010.
    • Y. Fujii, M. Kowaka, and A. Onodera, J. Phys. C 0022-3719 10.1088/0022-3719/18/4/010 18, 789 (1985).
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    • Fujii, Y.1    Kowaka, M.2    Onodera, A.3
  • 14
    • 63649140236 scopus 로고    scopus 로고
    • The amorphous state found previously happened to be the high-pressure state, so we named this state Am-I.
    • The amorphous state found previously happened to be the high-pressure state, so we named this state Am-I.
  • 18
    • 4544376934 scopus 로고    scopus 로고
    • The flatness of the melting curve cannot be explained, even by incorporating the effect of multipolar interactions to the intermolecular interaction. We concluded that the rigidity of molecules can no longer be assumed adequate for describing the system under pressures beyond 1 GPa. See,. 0038-1098
    • The flatness of the melting curve cannot be explained, even by incorporating the effect of multipolar interactions to the intermolecular interaction. We concluded that the rigidity of molecules can no longer be assumed adequate for describing the system under pressures beyond 1 GPa. See K. Fuchizaki and K. Nagai, Solid State Commun. 132, 305 (2004). 0038-1098
    • (2004) Solid State Commun. , vol.132 , pp. 305
    • Fuchizaki, K.1    Nagai, K.2
  • 21
    • 63649156192 scopus 로고    scopus 로고
    • This is explicitly expressed by Sintra (k) =1+ 8 5 j0 (k rSn-I) + 12 5 j0 (8 3 k rSn-I), where rSn-I is an intramolecular distance between Sn and I, and j0 denotes the zeroth-order spherical Bessel function.
    • This is explicitly expressed by Sintra (k) =1+ 8 5 j0 (k rSn-I) + 12 5 j0 (8 3 k rSn-I), where rSn-I is an intramolecular distance between Sn and I, and j0 denotes the zeroth-order spherical Bessel function.
  • 22
    • 63649094772 scopus 로고    scopus 로고
    • A constraint was imposed on the code developed in Ref. so that the shape of the MD cell, which contains 216 molecules, remains cubic.
    • A constraint was imposed on the code developed in Ref. so that the shape of the MD cell, which contains 216 molecules, remains cubic.
  • 23
    • 63649128197 scopus 로고    scopus 로고
    • The intermolecular interaction was tuned to reproduce the compressibility of CP-I at RT (Ref.). No readjustment of the parameters included in the intermolecular potential was made. We examined liquid structures along the melting curve of the model liquid and found that the model liquid at 1.3 GPa, 1500 K captures well the structural characteristics of the real liquid at 0.4 GPa, 610 K.
    • The intermolecular interaction was tuned to reproduce the compressibility of CP-I at RT (Ref.). No readjustment of the parameters included in the intermolecular potential was made. We examined liquid structures along the melting curve of the model liquid and found that the model liquid at 1.3 GPa, 1500 K captures well the structural characteristics of the real liquid at 0.4 GPa, 610 K.
  • 26
    • 0141843497 scopus 로고    scopus 로고
    • 0953-8984 10.1088/0953-8984/15/36/304,. However, ΔS19 J mole-1 K-1, which is also much larger than that expected in supercooled water, was reported for a polyamorphic transition in supercooled liquid yttria alumina (Ref.).
    • E. G. Ponyatovsky, J. Phys.: Condens. Matter 0953-8984 10.1088/0953-8984/15/36/304 15, 6123 (2003). However, ΔS19 J mole-1 K-1, which is also much larger than that expected in supercooled water, was reported for a polyamorphic transition in supercooled liquid yttria alumina (Ref.).
    • (2003) J. Phys.: Condens. Matter , vol.15 , pp. 6123
    • Ponyatovsky, E.G.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.