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Effect of pressure on the dielectric behavior of a bent-core liquid crystal
Phys. Rev. E 87, 042504 – Published 19 April, 2013
DOI: https://doi.org/10.1103/PhysRevE.87.042504
Abstract
We report the effect of applied pressure on the dielectric properties of the 2 phase of a bent-core liquid crystal. This study on bent-core banana-shaped molecules shows that while the dielectric anisotropy hardly varies with pressure, the relaxation parameters associated with the rotation around the long axes of the molecules are significantly influenced. These studies also bring out the fact that there are additional phases between the 2 phase and the true crystalline solid. Indeed, the existence of another variant of the 2 phase (labeled ), is revealed only in dielectric studies but not seen in x-ray and calorimetric measurements. Employing the dependence of the relaxation frequency along isobaric as well as isothermal paths, different activation parameters are determined and their behavior is compared with those of rodlike systems. The influence of dc bias on the dielectric behavior obtained at atmospheric pressure is also presented, which exhibits features similar to chiral antiferroelectric smectics, and further shows an additional relaxation over a small window of dc voltages.
Article Text
References (29)
- Thermotropic Liquid Crystals: Recent Advances, edited by A. Ramamoorthy (Springer, Dordrecht, 2010), Chaps. 1, 2.
- D. R. Link, G. Natale, R. Shao, J. E. Maclennan, N. A. Clark, E. Körblova, and D. M. Walba, Science 278, 1924 (1997).
- R. A. Reddy and C. Tschierske, J. Mater. Chem. 16, 907 (2006).
- H. Takezoe and Y. Takanishi, Jpn. J. Appl. Phys., Suppl. 45, 597 (2006).
- W. Weissflog, I. Wirth, S. Diele, G. Pelzl, H. Schmalfuss, T. Schoss, and A. Würflinger, Liq. Cryst. 28, 1603 (2001).
- S. Krishna Prasad, Y. Maeda, D. S. Shankar Rao, S. A. Nagamani, U. S. Hiremath, and C. V. Yelamaggad, Liq. Cryst. 30, 1277 (2003).
- C. V. Yelamaggad, U. S. Hiremath, S. A. Nagamani, D. S. Shankar Rao, and S. Krishna Prasad, J. Mater. Chem. 11, 1818 (2001).
- P. N. Bapat, D. S. Shankar Rao, S. Krishna Prasad, and C. V. Yelamaggad, J. Phys. Chem. B 114, 12825 (2010).
- It should be borne in mind that in the present case the system exhibits a direct transition from the isotropic to the tilted polar smectic (2) phase. In such cases, the antiferroelectric order appears simultaneously with not only the orientational nematic order but also the one- positional smectic density wave at the same thermally strong first order transition. Thus, the tilt angle can be expected to be essentially very high (see, e.g., Chap. 1 of Ref. [1]) and temperature independent except in the close proximity of the isotropic phase. In a similar situation, for systems with direct isotropic to smectic transition it is presumed that the tilt angle in the smectic phase is completely determined by the nematic order parameter; P. K. Mukherjee, H. Pleiner, and H. R. Brand, J. Chem. Phys. 117, 7788 (2002); Indeed, the suggestion from these two statements that the order parameter for the 2 phase is high is corroborated by NMR studies on smectic phases in bent-core systems; W. Weissflog, U. Baumeister, M. G. Tamba, G. Pelzl, H. Kresse, R. Friedemann, G. Hempel, R. Kurz, M. Roos, K. Merzweiler, A. Jákli, C. Zhang, N. Diorio, R. Stannarius, A. Eremin, and U. Korneket, Soft Matter 8, 2671 (2012).
- See, e.g., B. R. Ratna, M. S. Vijaya, R. Shashidhar, and B. K. Sadashiva, Liq. Cryst., Proc. Int. Conf. (1973), Pramana Suppl. 1, 69 (1975); N. V. Madhusudana and S. Chandrasekhar, ibid. 1, 57 (1975); M. J. Bradshaw and E. P. Raynes, Mol. Cryst. Liq. Cryst., Lett. Sect. 72, 73 (1981); S. Sridevi, S. Krishna Prasad, D. S. Shankar Rao, and C. V. Yelamaggad, J. Phys.: Condens. Matter 20, 465106 (2008).
- S. Urban and A. Wurflinger, in Advances in Chemical Physics, edited by I. Prigogine (John Wiley and Sons, Inc., New York, 1997).
- S. Krishna Prasad, in The Encyclopedia of Materials: Science and Technology, edited by K. H. J. Buschow, R. Cahn, M. Flemings, B. Ilschner, E. Kramer, S. Mahajan, and P. Veyssiere (Elsevier Science Ltd., Amsterdam, 2001).
- Y. Maeda, D. S. Shankar Rao, S. Krishna Prasad, S. Chandrasekar, and S. Kumar, Liq. Cryst. 28, 1679 (2001).
- A. Molenberg, M. Moller, and E. Sautter, Prog. Polym. Sci. 22, 1133 (1997).
- D. S. Shankar Rao, V. K. Gupta, S. Krishna Prasad, M. Manickam, and S. Kumar, Mol. Cryst. Liq. Cryst. 319, 193 (1998).
- V. N. Raja, R. Shashidhar, S. Chandrasekhár, R. E. Boehm, and D. E. Martire, Pramana 25, L119 (1985).
- J. M. Buisine, J. Malthete, C. Destrade, and N. H. Tinh, Phys. B (Amsterdam, Neth.) 139-140, 631 (1986).
- S. Chandrasekhar, B. K. Sadashiva, K. A. Sursh, N. V. Madhushdana, S. Kumar, R. Shashidhar, and G. Venkatesh, J. Phys., Colloq. 40, C3-120 (1979).
- Prasad N. Bapat, D. S. Shankar Rao, S. Krishna Prasad, and U. S. Hiremath, Thermochim. Acta 537, 65 (2012).
- S. Havriliak and S. Negami, J. Polym. Sci., Part C: Polym. Lett. 14, 99 (1966).
- S. Diele, S. Grande, H. Kruth, C. H. Lischk, G. Pelzl, W. Weissflog, and I. Wirth, Ferroelectrics 212, 169 (1998).
- H. Nadasi, W. Weissflog, A. Eremin, G. Pelzl, S. Diele, B. Das, and S. Grande, J. Mater. Chem. 12, 1316 (2002).
- A. Eremin, I. Wirth, S. Diele, G. Pelzl, H. Schmalfuss, H. Kresse, H. Nádasi, K. Fodor-Csorba, E. Gács-Baitz, and W. Weissflog, Liq. Cryst. 29, 775 (2002).
- S. Urban and C. M. Roland, J. Non-Cryst. Solids 357, 740 (2011).
- K. L. Sandhya, D. S. Shankar Rao, S. Krishna Prasad, U. S. Hiremath, and C. V. Yelamaggad, Thermochim. Acta 452, 65 (2007).
- M. Sandmann, D. Busing, T. Bruckert, A. Wurflinger, S. Urban, and B. Gestblom, SPIE 3318, 223 (1998).
- A. Fukuda, Y. Takanishi, T. Isozaki, K. Ishikawa, and H. Takezoe, J. Mater. Chem. 4, 997 (1994).
- A. Mukherjee, S. S. Bhattacharyya, M. Marik, B. K. Chaudhuri, and K. C. Majumdar, Phase Transitions 84, 908 (2011).
- Z. Vakhovskay, W. Weissflog, R. Friedemann, and H. Kresse, Phase Transitions 80, 705 (2007); S. Wróbel, J. Chruściel, M. Wierzejska-Adamowicz, M. Marzec, D. M. Ossowska-Chruściel, C. Legrand, and R. Douali, in Ferroelectrics—Physical Effects, edited by M. Lallart (InTech, Rijeka, Croatia, 2011), http://www.intechopen.com/books/ferroelectrics-physical-effects/ferroelectric-liquid-crystals-composed-of-banana-shaped-thioesters; J. K. Song, U. Manna, A. Fukuda, and J. K. Vij, Appl. Phys. Lett. 93, 142903 (2008); K. Hiraoka, H. Takezoe, and A. Fukuda, Ferroelectrics 147, 13 (1993); K. Hiraoka, A. D. L. Chandani, E. Gorecka, Y. Ouchi, H. Takezoe, and A. Fukuda, Jpn. J. Appl. Phys. 29, L1473 (1990).