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首页> 外文期刊>Ferroelectrics >Spontaneous polarization, tilt angle, hysteresis and low-frequency relaxations in hydrogen bonded chiral liquid crystal dimer: M*SA:9OBA
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Spontaneous polarization, tilt angle, hysteresis and low-frequency relaxations in hydrogen bonded chiral liquid crystal dimer: M*SA:9OBA

机译:氢键合手性液晶二聚体中的自发极化,倾斜角,滞后和低频松弛:M * SA:9oba

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Influence of low-frequency (2-Hz-10MHz) AC field on LC phases exhibited by chiral hydrogen bonded liquid crystal dimer, viz., M*SA:9OBA is investigated. Phase transition temperatures T-c determined by capacitance C(T) and loss factor Tan Delta(T) agree with the earlier report. Induced surface polarization reflected through capacitance C(E) exhibited hysteresis in behavior SmC* phase. Growth of primary order parameter in SmC* phase investigated by tilt angle theta(T) inferred critical field exponent beta(1). Secondary order parameter investigated as spontaneous polarization P-s in SmC* inferred Mean field exponent beta(2). Dipole moment (mu) is resolved as longitudinal (mu(l)) and transverse (mu(t)) components. Reorientation of mu to the field analyzed. Relaxation studied at different temperatures in SmC*; SmBcryst and SmG phases inferred a low-frequency (LF f(R)similar to 100Hz) and another high frequency (HF f(R)similar to 100kHz) reorientation processes. LF relaxation in SmC* phase is influenced by dc bias field to suggest polarization helix formed by coupling of field mu(t). Threshold field (V-th) for polarization switching estimated from the data of field variation of loss epsilon(max)''(E). LF relaxation in SmC* is identified with Goldstone mode (GM) manifested as the suppressed epsilon ''(max)(E) with field. HF relaxation in SmC* is identified with Soft Mode (SM) by its decreasing trend of f(R) towards T-IC*. Activation energies (E-a) estimated from Arrhenius behavior of f(R)(T) agree with reports. Field influence on GM manifests through shift of loss epsilon ''(max)(E) and f(R)(E). Activation energy E-a is estimated from the shift of f(R)(E) in terms of equivalent temperature plots. Dispersion, epsilon '' versus epsilon ' in LC phases infers a non-Debye distribution of relaxation times. Cole-Cole plots inferred large shift of static permittivity epsilon(o). Data of dielectric relaxation parameters, i.e., relaxation frequency f(R), relaxation time tau(R), activation energy E-a, loss maxima epsilon ''(max), static permittivity (epsilon(o)), high frequency permittivity epsilon(infinity), dielectric strength Delta epsilon and distribution (alpha) parameter are presented. Dielectric strength analyzed for SM in SmC* phase confirms Ferro-Electric Curie-Weiss behavior.
机译:低频(2-HZ-10MHz)交流场对手性氢键合液晶二聚体,Viz表现出的LC阶段的影响。,M * SA:9oba。通过电容C(t)和损耗因子Tan delta(t)决定的相变温度T-C与早期的报告一致。通过电容C(e)反射的诱导表面偏振表现出行为SMC *相中的滞后。通过倾斜角度θ(t)调查的SMC *阶段中主要订单参数的生长推断临界场指数β(1)。次要订单参数在SMC *推断平均场指数β(2)中被调查为自发极化P-S。偶极力矩(mu)被分解为纵向(mu(l))和横向(mu(t))组件。分析亩的亩。放松在SMC *的不同温度下研究; SMBCRYST和SMG阶段推断出低频(类似于100Hz的LF F(R))和另一种高频(类似于100kHz的HF F(R))的重新定位过程。 SMC *相中的LF弛豫受DC偏置场的影响,以建议通过耦合磁场MU(T)形成的偏振螺旋。阈值场(第V-T)从损耗epsilon(max)''(e)的场变形数据估计的偏振切换。 SMC *中的LF放松是用Goldstone模式(GM)识别,表现为抑制ε''(MAX)(E)与现场。 SMC *中的HF弛豫*通过其向T-IC *的F(R)的趋势降低而识别了软模式(SM)。从F(R)(T)的Arhenius行为估计的激活能量(E-A)同意报告。通过损失ε'(MAX)(E)(E)和F(e)偏移的转变对Gm表现的影响。在等效温度图方面,从F(r)(e)的偏移估计激活能量E-A. D分散,LC阶段的epsilon'与epsilon'infers infers的弛豫时间分布。 COLE-COLE图推断出静电渗透度ε(O)的大移位。介电弛豫参数,即松弛频率f(r),弛豫时间tau(r),激活能量ea,损失Maxima epsilon''(MAX),静电介电常数(epsilon(o)),高频介电常数ε(无限远),提出了介电强度δε和分布(alpha)参数。 SMC *相中SM分析的介电强度证实铁电居民威丝行为。

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