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Numéro
J. Phys. II France
Volume 4, Numéro 4, April 1994
Page(s) 581 - 588
DOI https://doi.org/10.1051/jp2:1994149
References of J. Phys. II France 4 581-588
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  8. In the previous reports, this phase has been termed S c2 phase, but S c2 is a confusing notation in the context of the nomenclature described in low molar mass systems. For this reason, we will hereafter adopt the notation of S c2 which has been adopted for the same type of smectic phase in low molar mass system by Fukuda et al.; Chandani A.D.L., Gorecka E., Ouchi Y., Takezoe H. and Fukuda A., Jpn J. Appl. Phys. 28 (1989) L1265 [CrossRef].
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  12. It should be noted here that this space group is essentially different from that of the S $_{\scriptsize\textrm{Ca}}$ phase which is analogous to the crystallographic D52h [4, 11].
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  18. It should noted here that the fundamental bilayer smectic phase has a biaxial character and so another frustrated structure can be also proposed such that the unusual density modulation occurs in a direction perpendicular to the tilt direction. In the present time, we cannot select one of these two models since the X-ray pattern has been observed only for the fiber specimen. However, even if any model is adopted, the structural characteristics described here are not essentially altered.
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