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Volumn 109, Issue 6, 1998, Pages 2361-2370

A theory for the liquid-crystalline phase behavior of the Gay-Berne model

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[No Author keywords available]

Indexed keywords


EID: 0000161378     PISSN: 00219606     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.476804     Document Type: Article
Times cited : (55)

References (26)
  • 16
    • 0009254419 scopus 로고
    • A fluid of perfectly aligned HGO molecules can be made thermodynamically equivalent to a fluid of hard spheres by appropriate scaling along the direction of alignment [see
    • A fluid of perfectly aligned HGO molecules can be made thermodynamically equivalent to a fluid of hard spheres by appropriate scaling along the direction of alignment [see J. L. Lebowitz and J. W. Perram, Mol. Phys. 50, 1207 (1983), who discussed this point for hard ellipsoids of revolution]. Since hard spheres do not exhibit phases intermediate between the fluid and the three-dimensional crystal, a smectic phase should not exist in the HGO system.
    • (1983) Mol. Phys. , vol.50 , pp. 1207
    • Lebowitz, J.L.1    Perram, J.W.2
  • 26
    • 22244445871 scopus 로고    scopus 로고
    • ′=5 has been calculated previously (Ref. 6) using a perturbative theory related to the one presented here but slightly more sophisticated (WCA splitting of the potential, introduction of an approximate reference radial distribution function, and full minimization of the one-molecule distribution function). This theory, however, is not suitable to describe the smectic phase.
    • ′=5 has been calculated previously (Ref. 6) using a perturbative theory related to the one presented here but slightly more sophisticated (WCA splitting of the potential, introduction of an approximate reference radial distribution function, and full minimization of the one-molecule distribution function). This theory, however, is not suitable to describe the smectic phase.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.