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A).
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Examples of columnar phases formed by bent-core molecules: (a) Watanabe, J.; Niori, T.; Sekine, T.; Takezoe, H. Jpn. J. Appl. Phys. 1998, 37, L139-L142.
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Examples of columnar phases formed by bent-core molecules: (a) Watanabe, J.; Niori, T.; Sekine, T.; Takezoe, H. Jpn. J. Appl. Phys. 1998, 37, L139-L142.
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mol corrected for the less dense packing in the liquid crystal assuming the packing coefficient to be intermediate between the average packing coefficient in the crystalline (k = 0.7) and liquid state (k = 0.55) (Kitaigorodski, A. I. Molekülkristalle, Akademieverlag Berlin, 1979, see Table S2).
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mol corrected for the less dense packing in the liquid crystal assuming the packing coefficient to be intermediate between the average packing coefficient in the crystalline (k = 0.7) and liquid state (k = 0.55) (Kitaigorodski, A. I. "Molekülkristalle", Akademieverlag Berlin, 1979, see Table S2).
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Examples of polar switching columnar phases of non-silylated compounds: (a) Reddy, R. A.; Sadashiva, B. K.; Baumeister, U. J. Mater. Chem. 2005, 15, 3303-3316.
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Examples of polar switching columnar phases of non-silylated compounds: (a) Reddy, R. A.; Sadashiva, B. K.; Baumeister, U. J. Mater. Chem. 2005, 15, 3303-3316.
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(b) Umadevi, S.; Sadashiva, B. K.; Shreenivasa Murthy, H. N.; Raghunathan, V. A. Soft Matter 2006, 2, 210-214.
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(d) Weissflog, W.; Naumann, G.; Kosata, B.; Schröder, M. W.; Eremin, A.; Diele, S.; Vakhovskaya, Z.; Kresse, H.; Friedemann, R.; Ananda Ramakrishnan, S.; Pelzl, G. J. Mater. Chem. 2005, 15, 4328-4337.
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Ananda Ramakrishnan, S.10
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Coleman, D. A.; Fernsler, J.; Chattham, N.; Nakata, M.; Takanishi, Y.; Korblova, E.; Link, D. R.; Shao, R.-F.; Jang, W. G.; Maclennan, J. E.; Mondainn-Monval, O.; Boyer, C.; Weissflog, W.; Pelzl, G.; Chien, L.-C.; Zasadzinski, J.; Watanabe, J.; Walba, D. M.; Takezoe H.; Clark, N. A. Science 2003, 301, 1204-1211.
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Coleman, D.A.1
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Mondainn-Monval, O.11
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more..
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79
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33947112704
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In the ColobPFE phases of 4a and 5a the splay seems to be relatively weak, as it can be removed under an electric field, leading to a FE switching smectic phase. Also, formation of an oblique lattice instead of a rectangular one is in line with a relatively weak splay of polarization
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FE phases of 4a and 5a the splay seems to be relatively weak, as it can be removed under an electric field, leading to a FE switching smectic phase. Also, formation of an oblique lattice instead of a rectangular one is in line with a relatively weak splay of polarization.
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80
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(a) Pelzl, G.; Diele, S.; Jakli, A.; Lischka, C.; Wirth, I.; Weissflog, W. Liq. Cryst. 1999, 26, 135-139.
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Pelzl, G.1
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85
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(e) Dunemann, U.; Schröder, M. W.; Reddy, R. A.; Pelzl, G.; Diele, S.; Weissflog, W. J. Mater. Chem. 2005, 15, 4051-4061.
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Dunemann, U.1
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Pelzl, G.4
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Weissflog, W.6
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86
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4744363280
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(f) Pelzl, G.; Schröder, M. W; Dunemann, U.; Diele, S.; Weissflog, W.; Jones, C.; Coleman, D.; Clark, N.A.; Stannarius, R.; Li, J.; Dasc, B.; Grande, S. J. Mater. Chem. 2004, 14, 2492-2498.
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Pelzl, G.1
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Jones, C.6
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Stannarius, R.9
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Dasc, B.11
Grande, S.12
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87
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37649031301
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7-type phases: Nakata, M.; Link, D. R.; Takanishi, Y.; Takahasi, Y.; Thisayukta, J.; Niwano.H. Coleman, D.A.; Watanabe, J.; Iida, A.; Clark, N. A.; Takezoe, H. Phys. Rev. E 2005, 71, 011705.
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7-type phases: Nakata, M.; Link, D. R.; Takanishi, Y.; Takahasi, Y.; Thisayukta, J.; Niwano.H. Coleman, D.A.; Watanabe, J.; Iida, A.; Clark, N. A.; Takezoe, H. Phys. Rev. E 2005, 71, 011705.
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88
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Examples of field-induced Col to Sm transitions: (a) Ortega, J.; de la Fuente, M. R.; Etxebarria, J.; Folcia, C. L.; Diez, S.; Gallastegui, J. A.; Gimeno, N.; Ros, M. B. Phys. Rev. E 2004, 69, 011703.
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Examples of field-induced Col to Sm transitions: (a) Ortega, J.; de la Fuente, M. R.; Etxebarria, J.; Folcia, C. L.; Diez, S.; Gallastegui, J. A.; Gimeno, N.; Ros, M. B. Phys. Rev. E 2004, 69, 011703.
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(b) Etxebarria, J.; Folcia, C. L.; Ortega, J.; Ros, M. B. Phys. Rev. E 2003, 67, 042702.
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Etxebarria, J.1
Folcia, C.L.2
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Ros, M.B.4
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90
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33947123010
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FE switching on a cone is in principle possible in flat layers as well as in modulated and undulated layers. In contrast, in AF switching modulated (columnar) phases the switching on a cone is hindered for steric reasons an unfavorable packing would arise at the inter-ribbon interfaces, and therefore, switching around the molecular long axis is observed instead of the switching on a cone
-
FE switching on a cone is in principle possible in flat layers as well as in modulated and undulated layers. In contrast, in AF switching modulated (columnar) phases the switching on a cone is hindered for steric reasons (an unfavorable packing would arise at the inter-ribbon interfaces), and therefore, switching around the molecular long axis is observed instead of the switching on a cone.
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91
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33344469328
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FE switching by rotation on a cone was also observed for a FE switching columnar phase of bent-core dimesogens: Umadevi, S, Jakli, A, Sadashiva, B. K. Soft Matter 2006, 2, 215-222
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FE switching by rotation on a cone was also observed for a FE switching columnar phase of bent-core dimesogens: Umadevi, S.; Jakli, A.; Sadashiva, B. K. Soft Matter 2006, 2, 215-222.
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2442639044
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Examples for switching of suprastructural chirality by collective rotation around the long axis: (a) Schröder, M. W.; Diele, S.; Pelzl, G.; Weissflog, W. ChemPhysChem 2004, 5, 99-103.
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Examples for switching of suprastructural chirality by collective rotation around the long axis: (a) Schröder, M. W.; Diele, S.; Pelzl, G.; Weissflog, W. ChemPhysChem 2004, 5, 99-103.
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94
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(c) Reddy, R. A.; Schröder, M. W.; Bodyagin, M.; Kresse, H.; Diele, S.; Pelzl, G.; Weissflog, W. Angew. Chem., Int. Ed. 2005, 44, 774-778.
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95
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15244355528
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(d) Weissflog, W.; Dunemann, U.; Schröder, M. W.; Diele, S.; Pelzl, G.; Kresse, H.; Grande, S. J. Mater. Chem. 2005, 15, 939-946.
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(e) Nakata, M.; Shao, R. F.; Maclennan, J.; Weissflog, W.; Clark, N. A. Phys. Rev. Lett. 2006, 96, 067802.
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Nakata, M.1
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Clark, N.A.5
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97
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33947144540
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This mesophase stabilizing effect was also observed for compounds of structure 2 (Chart 1),8d.20,21,30 whereas in calamitic mesogens lateral F substituents usually reduce the transition temperatures: Takeshi, I. In Organofluorine Chemistry: Principles and Commercial Applications; Banks, R.E, et al, Eds, Plenum Press: New York, 1994; pp 263-286
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8d.20,21,30 whereas in calamitic mesogens lateral F substituents usually reduce the transition temperatures: Takeshi, I. In Organofluorine Chemistry: Principles and Commercial Applications; Banks, R.E., et al., Eds.; Plenum Press: New York, 1994; pp 263-286.
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Liao, G.; Stojadinovic, S.; Pelzl, G.; Weissflog, W.; Sprunt, S.; Jákli, A. Phys. Rev. E, 2005, 72, 021710.
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Liao, G.1
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Sprunt, S.5
Jákli6
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99
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33947127514
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aPA structure obtained at 0 V should be the same as that proposed for the dark conglomerate textures in the ground state of these mesophases with the difference that it is not optically isotropic.
-
aPA structure obtained at 0 V should be the same as that proposed for the dark conglomerate textures in the ground state of these mesophases with the difference that it is not optically isotropic.
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100
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0141573132
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(a) Folcia, C. L.; Ortega, J.; Etxebarria, J. Liq. Cryst. 2003, 30, 1189-1191.
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Folcia, C.L.1
Ortega, J.2
Etxebarria, J.3
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101
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4744358746
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(b) Pyc, P.; Mieczkowski, J.; Pociecha, D.; Gorecka, E.; Donnio, B.; Guillon, D. J. Mater. Chem. 2004, 14, 2374-2379.
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J. Mater. Chem
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Pyc, P.1
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Gorecka, E.4
Donnio, B.5
Guillon, D.6
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102
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33947176986
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The smooth texture under the applied field (Figure 13b) is replaced by a stripe texture at 0 V Figure 13c, Such stripe pattern could have different reasons. One possibility is that the size of the [SmCsP F]sPA domains under the field is larger than the size of the SmCsPF layer stacks in the [SmC sPF]sPA structure at 0 V
-
A structure at 0 V.
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103
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33947120534
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The absence of an odd-even effect (see ref 12) is an additional indication of the week coupling between the layers
-
The absence of an odd-even effect (see ref 12) is an additional indication of the week coupling between the layers.
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