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- Kim , K. H. , Takanishi , Y. , Ishikawa , K. , Takezoe , H. and Fukuda , A. 1994 . Liq. Cryst. , 16 : 185 In this article, they concluded that peak (b) occured below (not at) the phase transition temperature from the higher temperature solid to SC A∗, because they observed crystalline patterns of the Raman spectra in the temperature range between peaks (b) and (d). However, it is reasonable that the crystalline patterns were observed in the temperature range, because the stabilization to a more stable crystalline state occurs at the exothermic peak (c) immediately following peak (b). We also reported crystalline patterns of X-ray diffraction in the same temperature range [5]. In addition, an endothermic peak (entropy increase such as chain melting) should be associated to any change of the gradient of the Gibbs energy (G), because of a general relation (ΔG/T)p = -ΔS. Thus, their microscopic interpretation that peak (b) is due to partial chain melting and our macroscopic interpretation that the change corresponds to the higher temperature solid to the SC A∗ phase transition are compatible
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