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Line tensions, correlation lengths, and critical exponents in lipid membranes near critical points.

机译:临界点附近脂质膜的线张力,相关长度和临界指数。

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摘要

Membranes containing a wide variety of ternary mixtures of high chain-melting temperature lipids, low chain-melting temperature lipids, and cholesterol undergo lateral phase separation into coexisting liquid phases at a miscibility transition. When membranes are prepared from a ternary lipid mixture at a critical composition, they pass through a miscibility critical point at the transition temperature. Since the critical temperature is typically on the order of room temperature, membranes provide an unusual opportunity in which to perform a quantitative study of biophysical systems that exhibit critical phenomena in the two-dimensional Ising universality class. As a critical point is approached from either high or low temperature, the scale of fluctuations in lipid composition, set by the correlation length, diverges. In addition, as a critical point is approached from low temperature, the line tension between coexisting phases decreases to zero. Here we quantitatively evaluate the temperature dependence of line tension between liquid domains and of fluctuation correlation lengths in lipid membranes to extract a critical exponent, nu. We obtain nu = 1.2 +/- 0.2, consistent with the Ising model prediction nu = 1. We also evaluate the probability distributions of pixel intensities in fluorescence images of membranes. From the temperature dependence of these distributions above the critical temperature, we extract an independent critical exponent of beta = 0.124 +/- 0.03, which is consistent with the Ising prediction of beta = 1/8.
机译:包含高链熔点温度脂质,低链熔点温度脂质和胆固醇的多种三元混合物的膜在可混溶转变时经历侧向相分离成共存的液相。当膜由临界组成的三元脂质混合物制备时,它们会在转变温度下通过溶混性临界点。由于临界温度通常在室温左右,因此膜提供了一个难得的机会,可以对生物物理系统进行定量研究,以显示二维Ising通用性类别中的临界现象。当从高温或低温接近临界点时,由相关长度设定的脂质组成波动的规模不同。另外,随着从低温接近临界点,共存相之间的线张力减小到零。在这里,我们定量评估液域之间的线张力和脂质膜中波动相关长度的温度依赖性,以提取临界指数nu。我们获得nu = 1.2 +/- 0.2,与Ising模型的预测nu = 1一致。我们还评估了膜荧光图像中像素强度的概率分布。从高于临界温度的这些分布的温度依赖性,我们提取了一个独立的临界指数β= 0.124 +/- 0.03,这与伊辛预测的β= 1/8一致。

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