首页> 外文期刊>Liquid Crystals: An International Journal in the Field of Anisotropic Fluids >Low-temperature dynamics of (S)-4-(1-methylheptyloxy)-4 ' cyanobiphenyl (8*OCB) and (S)-4-(2-methylbutyl)-4 '-cyanobiphenyl (5*CB) in disordered crystalline and glassy phases
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Low-temperature dynamics of (S)-4-(1-methylheptyloxy)-4 ' cyanobiphenyl (8*OCB) and (S)-4-(2-methylbutyl)-4 '-cyanobiphenyl (5*CB) in disordered crystalline and glassy phases

机译:(S)-4-(1-甲基二氧基)-4''氰基溴苯基(8 * OCB)和(S)-4-(2-甲基丁基)-4'-CYAnbiphenyl(5 * CB)的低温动力学 和玻璃阶段

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摘要

The inelastic neutron scattering (INS) spectra were measured for two materials of chiral molecules: (S)-4-(1-methylheptyloxy)-4'-cyanobiphenyl (8*OCB) and (S)-4-(2-methylbutyl)-4'-cyanobiphenyl (5*CB), revealing solid state polymorphism with two partially disordered crystalline phases I and II and glassy state of liquid and of crystalline phase in each substance. The experiments were performed in the energy range up to 30 mu eV in the temperature range from 4 to 35 K. For 8*OCB the elastic scans were measured as well up to 300 K illustrating well the phase diagram. For all solid phases of both substances in the mu eV range of INS spectra, the existence of the excess density of vibrational states over that typical for fully ordered crystalline phases was evidenced. Contribution of this so-called boson peak occurred to be much larger in glass of isotropic phase than in the phase II and glass of phase I of 8*OCB, while for 5*CB it was larger in the phase I and glass of phase II than in glass of cholesteric phase. The quasi-elastic broadening of elastic peak corresponding to stochastic reorientations in the ns time scale was detected for both substances. Comparison of the results obtained for glassy and crystalline phases of 8*OCB and 5*CB compounds have been given and confronted with those obtained previously in meV energy range.
机译:测量非弹性中子散射(INS)光谱,用于两种手性分子材料:(S)-4-(1-甲基庚二氧基)-4'-氰基溴基(8 * OCB)和(S)-4-(2-甲基丁) -4'-氰基溴苯基(5 * Cb),揭示具有两个部分紊乱的结晶阶段I和II和玻璃状液体和每种物质的结晶相的固态多态性。在4至35k的温度范围内的能量范围内进行实验在4至35k的温度范围内进行。对于8 * OCB,测量弹性扫描,如图300K所示的相位图。对于MU EV范围内的所有物质的所有固体相,证明了对完全有序结晶相的典型振动状态的过度密度。在各向同性相位玻璃中发生这种所谓的玻色子峰的贡献比在8 * ocb的II期和玻璃中的同学相中大得多,而5 * Cb在I II和II阶段的玻璃中较大而不是在胆甾醇阶段。对两种物质检测到NS时间尺度中随机重构的弹性峰值的拟弹性膨胀。已经给予了8 * OCB和5 * CB化合物的玻璃和结晶相获得的结果的比较,并与先前在MEV能量范围内获得的那些相反。

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