首页> 外文期刊>Physical review, E. Statistical physics, plasmas, fluids, and related interdisciplinary topics >Two experimental tests of a fluctuation-induced first-order phase transition: Intensity fluctuation microscopy at the nematic-smectic-A transition - art. no. 021702
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Two experimental tests of a fluctuation-induced first-order phase transition: Intensity fluctuation microscopy at the nematic-smectic-A transition - art. no. 021702

机译:波动引起的一阶相变的两个实验测试:向列-近原子-A跃迁的强度波动显微镜-art。没有。 021702

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We have developed a new, extremely sensitive real-space technique (intensity fluctuation microscopy) to probe the order of the nematic-smectic-A (NA) transition. Using this technique, we show that the NA transition in 4'-n-octyl-4-cyanobiphenyl (8CB) is clearly first order, contrary to calorimetric studies but in agreement with conclusions drawn from front-velocity measurements. We characterize the strength of the discontinuity at the first-order transition by the dimensionless quantity t(0)=(T-NA - T*)/T*. By precisely measuring t(0), we have made the first detailed tests of predictions based on the Halperin-Lubensky-Ma (HLM) theory of fluctuation-induced, first-order phase transitions. First, we explore the effect of an external magnetic field on the NA transition. Although modest fields (of order 10 T) are predicted to drive the weakly first-order transition in pure 8CB second order, we observe no such effect, we establish instead that the lower bound on this critical field is approximate to 30 T. Likewise, we observe no effect in mixtures of 8CB with its longer chemical homolog 4'-n-decyl-4-cyanobiphenyl (10CB). Second, we examine the dependence of t(0) as a function of 8CB-10CB mixture concentration and find that the data in mixtures with small nematic temperature range are well-fit by the parameters derived by Anisimov et al. based on calorimetric measurements. As we increase the nematic range (by using concentrations closer to pure 8CB), the measured t(0) deviates more and more from the HLM predictions. Smectic fluctuations, which are neglected in the HLM calculation, are an obvious candidate to explain such a discrepancy, but one's naive expectation is that they would reduce t(0) below the HLM levels. whereas the observed values are too large. However, a recent re normalization-group calculation concludes that smectic fluctuations. surprisingly, should indeed increase t(0), explaining the observations presented here. [References: 36]
机译:我们已经开发了一种新的,极其敏感的实空间技术(强度波动显微镜),以探索向列-近原子-A(NA)过渡的顺序。使用这项技术,我们表明,在4'-n-辛基-4-氰基联苯(8CB)中的NA跃迁显然是一阶的,这与量热研究相反,但与从前向速度测量得出的结论一致。我们用无量纲量t(0)=(T-NA-T *)/ T *表征一阶跃迁的不连续强度。通过精确测量t(0),我们基于Halperin-Lubensky-Ma(HLM)理论对波动引起的一阶相变进行了首次详细的预测测试。首先,我们探讨了外部磁场对NA跃迁的影响。尽管预计适度的场(10 T量级)会在纯8CB二阶中驱动弱的一阶跃迁,但我们没有观察到这种影响,而是确定了该临界场的下限约为30T。类似地,我们观察到8CB与更长的化学同系物4'-n-癸基-4-氰基联苯(10CB)的混合物没有作用。其次,我们研究了t(0)与8CB-10CB混合物浓度的关系,发现向列温度范围小的混合物中的数据与Anisimov等人得出的参数完全吻合。基于量热测量。随着我们增加向列范围(通过使用接近纯8CB的浓度),测得的t(0)越来越偏离HLM预测。在HLM计算中被忽略的近场波动是解释这种差异的明显候选者,但是人们的天真期望是它们会将t(0)降低到HLM水平以下。观测值太大。但是,最近的重新归一化组计算得出的结论是近晶波动。令人惊讶的是,确实应该增加t(0),解释了这里介绍的观察结果。 [参考:36]

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