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球形囊泡的涨落动力学:常规体相耗散受阻进入亚扩散弛豫

Fluctuation dynamics of spherical vesicles: frustration of regular bulk dissipation into subdiffusive relaxation.

作者信息

Arriaga Laura R, López-Montero Iván, Orts-Gil Guillermo, Farago Bela, Hellweg Thomas, Monroy Francisco

机构信息

Mechanics of Biological Membranes and Biorheology, Universidad Complutense de Madrid, 28040 Madrid, Spain.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2009 Sep;80(3 Pt 1):031908. doi: 10.1103/PhysRevE.80.031908. Epub 2009 Sep 21.

DOI:10.1103/PhysRevE.80.031908
PMID:19905147
Abstract

Spherical lipid vesicles obtained by the extrusion method are nonequilibrium membrane structures more curved than the zero spontaneous curvature equilibrium state of the bilayer. Furthermore, these structures are quite rigid as compared to spontaneous vesicles or microemulsion droplets made of soluble surfactants. The dynamical description of the shape fluctuations derived by Milner and Safran (MS) [Phys. Rev. A 36, 4371 (1987)], which is based on the elastic Helfrich energy referred to the equilibrium state, could be misleading in these cases. In the present contribution, shape fluctuations of unilamellar palmitoyl-oleyl-phosphocholine (POPC) vesicles (radius Rh<or=100 nm ) prepared by extrusion are studied by means of neutron spin echo (NSE) in combination with dynamic light scattering (DLS). The relaxation of the fluctuation modes is inferred from the DLS autocorrelation functions and from the intermediate NSE scattering functions measured for several different values of the wave vector. The observed relaxations are compatible with a stretched-exponential decay rather than the single-exponential behavior. Dynamical frustration of the bulk dissipation mechanism in the way described by Zilman and Granek (ZG) for weak amplitude fluctuations [Phys. Rev. Lett. 77, 4788 (1996)] is invoked as a plausible scenario for explaining the subdiffusive nonexponential relaxations experimentally observed. The combined analysis of NSE and DLS data allows a calculation of the bending elastic constant of POPC vesicles kappa=19+/-2 kBT , in excellent agreement with literature data. The ZG approach is revealed as the adequate extension of the MS theory to describe fluctuation dynamics of rigid membranes.

摘要

通过挤压法获得的球形脂质囊泡是非平衡膜结构,其曲率比双层膜的零自发曲率平衡态更大。此外,与由可溶性表面活性剂制成的自发囊泡或微乳液滴相比,这些结构相当刚性。米尔纳和萨夫兰(MS)[《物理评论A》36, 4371 (1987)]基于参考平衡态的弹性赫尔弗里希能量推导的形状涨落动力学描述,在这些情况下可能会产生误导。在本论文中,通过中子自旋回波(NSE)结合动态光散射(DLS)研究了通过挤压制备的单层棕榈酰油酰磷脂酰胆碱(POPC)囊泡(半径Rh≤100 nm)的形状涨落。从DLS自相关函数以及针对几个不同波矢值测量的中间NSE散射函数推断涨落模式的弛豫。观察到的弛豫与拉伸指数衰减兼容,而不是单指数行为。齐尔曼和格拉内克(ZG)[《物理评论快报》77, 4788 (1996)]描述的弱振幅涨落情况下体耗散机制的动态受挫被作为解释实验观察到的亚扩散非指数弛豫的合理情景。NSE和DLS数据的联合分析允许计算POPC囊泡的弯曲弹性常数κ = 19±2 kBT,与文献数据非常吻合。ZG方法被证明是MS理论描述刚性膜涨落动力学的适当扩展。

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