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11
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0013413440
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to be published
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B. Das, S. Grande, A. Eremin, M. Schröder, S. Diele, G. Pelzl, H. Kresse, and W. Weissflog, Liq. Cryst. (to be published).
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Das, B.1
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Weissflog, W.8
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37649030979
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X.F. Han, D.A. Olson, A. Cady, J.W. Goodby, and C.C. Huang, Phys. Rev. E 65, 010704(R) (2002).
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D.A. Olson, X.F. Han, P.M. Johnson, A. Cady, and C.C. Huang, Liq. Cryst. 29, 1521 (2002).
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16
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0034506685
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If the compound exhibits the uniaxial Sm-A phase, the indices of refraction and the layer spacing can be measured by pulling a series of films in the Sm-A phase. Then N of any film can be determined. See P.M. Johnson, D.A. Olson, S. Pankratz, Ch. Bahr, J.W. Goodby, and C.C. Huang, Phys. Rev. E 62, 8106 (2000).
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Huang, C.C.6
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17
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0003972070
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Cambridge University Press, Cambridge
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The derivation for the transmission matrix which relates the incident and transmitted light can be found in M. Born and E. Wolf, Principles of Optics (Cambridge University Press, Cambridge, 1997). ψ is calculated from the equation given in Ref. [14].
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Principles of Optics
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Born, M.1
Wolf, E.2
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18
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0030576817
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D.R. Link, J.E. Maclennan, and N.A. Clark, Phys. Rev. Lett. 77, 2237 (1996); D.R. Link, G. Natale, N.A. Clark, J.E. Maclennan, M. Walsh, S.S. Keast, and M.E. Neubert, ibid. 82, 2508 (1999).
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Phys. Rev. Lett.
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Link, D.R.1
Maclennan, J.E.2
Clark, N.A.3
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19
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0001131483
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D.R. Link, J.E. Maclennan, and N.A. Clark, Phys. Rev. Lett. 77, 2237 (1996); D.R. Link, G. Natale, N.A. Clark, J.E. Maclennan, M. Walsh, S.S. Keast, and M.E. Neubert, ibid. 82, 2508 (1999).
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Phys. Rev. Lett.
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Link, D.R.1
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Walsh, M.5
Keast, S.S.6
Neubert, M.E.7
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20
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33645072116
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note
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The quality of the data obtained from the thin films is affected by the fact that there was a electroconvection flow of the material in the presence of E as was also reported in Ref. [8]. Nonetheless, as shown in Figs. 2(a) and 2(c), it is still possible to obtain conclusive data even under such conditions.
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-
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22
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0014664541
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If the tilt orientations of layers are not uniform along the layer normal, flexoelectric polarization exists. See R.B. Meyer, Phys. Rev. Lett. 22, 918 (1969). We cannot distinguish the flexoelectric polarization from the longitudinal polarization.
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(1969)
Phys. Rev. Lett.
, vol.22
, pp. 918
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Meyer, R.B.1
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23
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0000786817
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D.W. Berreman, J. Opt. Soc. Am. 62, 502 (1972); H. Wöhler, G. Haas, M. Fritsch, and D.A. Mlynski, J. Opt. Soc. Am. A 5, 1554 (1988).
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J. Opt. Soc. Am.
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, pp. 502
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Berreman, D.W.1
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24
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84912995886
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D.W. Berreman, J. Opt. Soc. Am. 62, 502 (1972); H. Wöhler, G. Haas, M. Fritsch, and D.A. Mlynski, J. Opt. Soc. Am. A 5, 1554 (1988).
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J. Opt. Soc. Am. A
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, pp. 1554
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Wöhler, H.1
Haas, G.2
Fritsch, M.3
Mlynski, D.A.4
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25
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33645048354
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note
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The optical parameters of DOBAMBC were measured with the method described in Ref. [16]. See Ref. [14] for details.
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26
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0000736169
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S. Dumrongrattana, C.C. Huang, G. Nounesis, S.C. Lien, and J.M. Viner, Phys. Rev. A 34, 5010 (1986).
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Phys. Rev. A
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Dumrongrattana, S.1
Huang, C.C.2
Nounesis, G.3
Lien, S.C.4
Viner, J.M.5
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27
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0010343527
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Movies to show the transitions in a 7-layer and ≈200-layer film can be found at http://groups.physics.umn.edu/lcrystal/DRLM/drlm.html. The thickness of thick films is estimated from their color. See E.B. Sirota, P.S. Pershan, L.B. Sorensen, and J. Collett, Phys. Rev. A 36, 2890 (1987).
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(1987)
Phys. Rev. A
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Sirota, E.B.1
Pershan, P.S.2
Sorensen, L.B.3
Collett, J.4
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28
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33645079551
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note
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2 phase [8]. However, such a structure implies that in even- (odd-) layer free-standing films, there should be a net polarization in (perpendicular to) the tilt plane [18]. Thus, the observation and proposal of Ref. [8] contradict each other.
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