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Volumn 66, Issue 3, 2002, Pages

Comparative x-ray and dielectric measurements of smectic A–smectic-[formula presented] transition in bulk and confined geometries

Author keywords

[No Author keywords available]

Indexed keywords

CRYSTALLINE MATERIALS; DIELECTRIC MATERIALS; ELECTROOPTICAL DEVICES; FERROELECTRIC MATERIALS; MOLECULAR DYNAMICS; MOLECULAR STRUCTURE; SOLVENTS; X RAY DIFFRACTION ANALYSIS;

EID: 41349084943     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.66.031710     Document Type: Article
Times cited : (22)

References (22)
  • 1
    • 85036260387 scopus 로고    scopus 로고
    • For an excellent collection of review articles in this field, see Liquid Crystals in Complex Geometries, edited by G. P. Crawford and S. Zumer (Taylor & Francis, London, 1996)
    • For an excellent collection of review articles in this field, see Liquid Crystals in Complex Geometries, edited by G. P. Crawford and S. Zumer (Taylor & Francis, London, 1996).
  • 9
    • 85036203721 scopus 로고    scopus 로고
    • F.M. Aliev, in Liquid Crystals in Complex Geometries, edited by G.P. Crawford and S. Zumer (Taylor & Francis, London, 1996), p. 345
    • F.M. Aliev, in Liquid Crystals in Complex Geometries, edited by G.P. Crawford and S. Zumer (Taylor & Francis, London, 1996), p. 345.
  • 15
    • 85036168672 scopus 로고    scopus 로고
    • Geetha G. Nair, S. Krishna Prasad, R. Shashidhar, B. R. Ratna, Ch. Bahr, and G. Heppke, Abstracts of the 13th International Liquid Crystal Conference, PHA-24, Vancouver, Canada, 1990 (unpublished)
    • Geetha G. Nair, S. Krishna Prasad, R. Shashidhar, B. R. Ratna, Ch. Bahr, and G. Heppke, Abstracts of the 13th International Liquid Crystal Conference, PHA-24, Vancouver, Canada, 1990 (unpublished).
  • 18
    • 0012016501 scopus 로고
    • The application of an electric field perpendicular to the layer normal direction in the chiral (Formula presented) phase leads to the appearance of an induced tilt. Thus, the two phases across the transition (which are (Formula presented) and (Formula presented) in the absence of the field) become isosymmetric. This situation is similar to that of a system with a gas-liquid transition. Consequently, there can only be a first-order transition between the two phases. In the (Formula presented) case, application of an electric field of certain strength results in a critical point, above which the two phases are indistinguishable and evolve continuously from one to another. For further details, see Ch. Bahr and G. Heppke, Phys. Rev. A 41, 4335 (1990).
    • (1990) Phys. Rev. A , vol.41 , pp. 4335
    • Bahr, C.1    Heppke, G.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.