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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書(shū)目名稱Atomic Dynamics in Liquids影響因子(影響力)




書(shū)目名稱Atomic Dynamics in Liquids影響因子(影響力)學(xué)科排名




書(shū)目名稱Atomic Dynamics in Liquids網(wǎng)絡(luò)公開(kāi)度




書(shū)目名稱Atomic Dynamics in Liquids網(wǎng)絡(luò)公開(kāi)度學(xué)科排名




書(shū)目名稱Atomic Dynamics in Liquids被引頻次




書(shū)目名稱Atomic Dynamics in Liquids被引頻次學(xué)科排名




書(shū)目名稱Atomic Dynamics in Liquids年度引用




書(shū)目名稱Atomic Dynamics in Liquids年度引用學(xué)科排名




書(shū)目名稱Atomic Dynamics in Liquids讀者反饋




書(shū)目名稱Atomic Dynamics in Liquids讀者反饋學(xué)科排名

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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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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.