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Volumn 66, Issue 4, 2002, Pages 8-

Effect of dispersed silica particles on the smectic-A–smectic-[formula presented] phase transition

Author keywords

[No Author keywords available]

Indexed keywords

AEROGELS; HYDROPHILICITY; SILICA; SMECTIC LIQUID CRYSTALS; SPECTROSCOPIC ANALYSIS; SUPERCONDUCTING TRANSITION TEMPERATURE;

EID: 41349097254     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.66.041702     Document Type: Article
Times cited : (64)

References (30)
  • 1
    • 85036293927 scopus 로고    scopus 로고
    • Liquid Crystals in Complex Geometries Formed by Polymer and Porous Networks, edited by G.P. Crawford and S. Žumer (Taylor and Francis, London, 1996)
    • Liquid Crystals in Complex Geometries Formed by Polymer and Porous Networks, edited by G.P. Crawford and S. Žumer (Taylor and Francis, London, 1996).
  • 3
    • 85036209408 scopus 로고    scopus 로고
    • P.G. de Gennes and J. Prost, The Physics of Liquid Crystals (Oxford University Press, Oxford, 1993)
    • P.G. de Gennes and J. Prost, The Physics of Liquid Crystals (Oxford University Press, Oxford, 1993).
  • 11
    • 85036405859 scopus 로고    scopus 로고
    • D.J. Cleaver, S. Kralj, T.J. Sluckin, and M.P. Allen, in Liquid Crystals in Complex Geometries Formed by Polymer and Porous Networks, edited by G.P. Crawford and S. Žumer (Taylor and Francis, London, 1996), p. 467
    • D.J. Cleaver, S. Kralj, T.J. Sluckin, and M.P. Allen, in Liquid Crystals in Complex Geometries Formed by Polymer and Porous Networks, edited by G.P. Crawford and S. Žumer (Taylor and Francis, London, 1996), p. 467.
  • 19
    • 85036176016 scopus 로고    scopus 로고
    • Degussa Corp., Silica Division, 65 Challenger Rd., Ridgefield Park, NJ 07660
    • Degussa Corp., Silica Division, 65 Challenger Rd., Ridgefield Park, NJ 07660.
  • 24
    • 85036140704 scopus 로고    scopus 로고
    • As far as the Goldstone mode frequency is concerned, no particular changes were observed up to (Formula presented) The magnitude of the Goldstone mode frequency further away from (Formula presented) remains to be in range (Formula presented) For (Formula presented) it slightly exceeds 3 kHz. However, it should be noted that at (Formula presented) the intensity of the Goldstone mode becomes very small in comparison to the soft mode. This makes the separation of two modes more difficult. The observed increase in the Goldstone mode frequency for (Formula presented) could easily be an artificial effect. Namely, the much larger high frequency soft mode could slightly bias the value of the Goldstone mode frequency during the two modes separation process
    • As far as the Goldstone mode frequency is concerned, no particular changes were observed up to (Formula presented) The magnitude of the Goldstone mode frequency further away from (Formula presented) remains to be in range (Formula presented) For (Formula presented) it slightly exceeds 3 kHz. However, it should be noted that at (Formula presented) the intensity of the Goldstone mode becomes very small in comparison to the soft mode. This makes the separation of two modes more difficult. The observed increase in the Goldstone mode frequency for (Formula presented) could easily be an artificial effect. Namely, the much larger high frequency soft mode could slightly bias the value of the Goldstone mode frequency during the two modes separation process.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.