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Titlebook: Atomic Dynamics in Liquids; N. H. March,M. P. Tosi Textbook 1976Latest edition N. H. March and M. P. Tosi 1976 collision.elastic scatterin

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发表于 2025-3-21 16:37:58 | 显示全部楼层 |阅读模式
期刊全称Atomic Dynamics in Liquids
影响因子2023N. H. March,M. P. Tosi
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图书封面Titlebook: Atomic Dynamics in Liquids;  N. H. March,M. P. Tosi Textbook 1976Latest edition N. H. March and M. P. Tosi 1976 collision.elastic scatterin
Pindex Textbook 1976Latest edition
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发表于 2025-3-21 21:43:55 | 显示全部楼层
Static Structure and Thermodynamics,natomic. In eqn (1.1), .(.) is the atomic scattering factor, i.e. the Fourier transform of the electron density in the atom. .(.) falls from a value ., the atomic number, at . = 0 to zero at large ., the asymptotic behaviour being proportional to ..
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Fuzzy Information and Engineering-2019ful for some purposes. We immediately confirm that, if we note that the ratio of the specific heats . for simple metals at their melting points is ∼1.2 or 1.3, whereas for a hard-sphere like system such as argon . ∼2.2 at the triple point.
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Xiuqin Xu,Jialiang Xie,Shuili Chenso Kubo, 1966). It will be instructive to introduce this formalism through a study of the simplest time-dependent correlation function, which is the velocity autocorrelation function for a particle in a classical fluid, before proceeding to the discussion of .(.).
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发表于 2025-3-23 06:56:21 | 显示全部楼层
Liquid Dynamics and Time-Dependent Correlation Functions,ent times. This function can be expressed in the form.The average of the . function involved in eqn (3.1) is obviously the probability that at time . the .th atom will be at . with respect to the position of the .th atom at time . = 0. We then sum this probability over . and average over .(.) is the space-time pair correlation function.
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