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85036260387
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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)
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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).
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7
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G.S Iannacchione, J.T. Mang, S. Kumar, and D. Finotello, Phys. Rev. Lett. 73, 2708 (1994).
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Iannacchione, G.S.1
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F.M. Aliev, in Liquid Crystals in Complex Geometries, edited by G.P. Crawford and S. Zumer (Taylor & Francis, London, 1996), p. 345
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F.M. Aliev, in Liquid Crystals in Complex Geometries, edited by G.P. Crawford and S. Zumer (Taylor & Francis, London, 1996), p. 345.
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10
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M. Skarabot, S. Kralj, R. Blinc, and I. Musevic, Liq. Cryst. 26, 723 (1999).
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S.A. Rozanski, R. Strannarius, F. Krenes, and S. Diele, Liq. Cryst. 28, 1071 (2001).
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J. Werner, K. Otto, D. Enke, G. Pelzl, F. Janowski, and H. Kresse, Liq. Cryst. 27, 1295 (2000).
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Werner, J.1
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13
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0035161351
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K.L. Sandhya, Geetha G. Nair, S. Krishna Prasad, and Anjuli Khandelwal, Liq. Cryst. 28, 1847 (2001).
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Sandhya, K.L.1
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Krishna Prasad, S.3
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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 Bahr, and G. Heppke, Abstracts of the 13th International Liquid Crystal Conference, PHA-24, Vancouver, Canada, 1990 (unpublished)
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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).
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H.Y. Liu, C.C. Huang, Ch. Bahr, and G. Heppke, Phys. Rev. Lett. 61, 345 (1998).
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Liu, H.Y.1
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Heppke, G.4
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18
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0012016501
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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).
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Phys. Rev. A
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Bahr, C.1
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S.U. Vallerien, F. Kramer, H. Kapitza, R. Zentel, and W. Frank, Phys. Lett. A 138, 219 (1989);
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S. Krishna Prasad, S.M. Khened, V.N. Raja, S. Chandrasekhar, and B. Shivakumar, Ferroelectrics 138, 37 (1993).
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Ferroelectrics
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