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首页> 外文期刊>The Journal of Chemical Physics >Effective charges along the melting line of colloidal crystals
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Effective charges along the melting line of colloidal crystals

机译:沿胶体晶体熔解线的有效电荷

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The shear modulus G of charged colloidal crystals was measured at several constant particle densities n and varying salt concentrations c up to the melting salt concentration c(M) using torsional resonance spectroscopy. Far from the phase boundary the samples are polycrystalline and the shear modulus stays roughly constant as a function of c. Upon approaching the melting transition an increasing amount of wall based crystal material is formed surrounding a shrinking polycrystalline core and G drops nearly linearly. When the transition is complete G again stays constant. The morphologic transitions may be scaled upon a single master curve. For the polycrystalline morphology, the elastic data are evaluated in terms of a pairwise additive screened Coulomb interaction yielding a particle effective charge Z(G)(*). Under de-ionized conditions Z(0,G)(*) is independent of n and significantly lower than expected from charge renormalization theory. With increasing salt concentration Z(G)(*) increases. The increase becomes more pronounced at larger n. By extrapolation we further obtain the melting line effective elasticity charge Z(M,G)(*). Z(M,G)(*) shows a steplike increase with increasing n(M) and c(M) to values consistent with charge renormalization theory. Interestingly, the increase coincides semi-quantitatively with the one expected from the universal melting line for charged spheres, thus facilitating a consistent description of phase behavior and elasticity over an extended range of the phase diagram. (c) 2006 American Institute of Physics.
机译:带电胶体晶体的剪切模量G是使用扭转共振光谱法在几个恒定的颗粒密度n和变化的盐浓度c直至熔融盐浓度c(M)下测量的。样品远离相界,是多晶的,剪切模量根据c保持大致恒定。在接近熔融转变时,围绕收缩的多晶核形成越来越多的壁基晶体材料,并且G几乎线性下降。转换完成后,G再次保持恒定。可以在单个主曲线上按比例缩放形态转变。对于多晶形态,根据成对加成物筛选的库仑相互作用评估弹性数据,产生颗粒有效电荷Z(G)(*)。在去离子条件下,Z(0,G)(*)与n无关,并且远低于电荷重整化理论的预期值。随着盐浓度的增加,Z(G)(*)增加。 n越大,增加越明显。通过外推,我们进一步获得了熔线有效弹性电荷Z(M,G)(*)。 Z(M,G)(*)随着n(M)和c(M)的增加呈逐步增加的趋势,达到与电荷重归一化理论一致的值。有趣的是,这种增加与带电球的通用熔解线所预期的增加相吻合,因此有助于在相图的扩展范围内对相行为和弹性进行一致的描述。 (c)2006年美国物理研究所。

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