Structure of Expanded Liquid Caesium in the Modified Hypernetted-Chain Approximation

Structure of liquid carbon tetrachloride up to the subcritical point measured by wide Q-range neutron diffraction

“…͑3͒ with a molecular center structure factor S c (Q) calculated from a PY hard sphere model, 22 because a repulsive potential alone does not give a significant density fluctuation. 23 The effective diameter of CCl 4 molecules estimated previously 12 is used by taking account of the temperature dependence. The net small angle scattering, S f (Q), is assumed to be given by subtracting S m u (Q) from the experimental S m (Q).…”

Universality in the structural change of expanded liquid alkali metals along the liquid-vapour coexistence curve

“…The structural properties of expanded liquid Rb have been studied by perturbation and integral-equation theories (Bratkovsky et af 1982, McLaughlin and Young 1984, Kahl and Hafner 1984, Gonzalez er a1 1990) and by simulations (Mountain 1978, Tanaka 1980 on the basisofthe effective pair potentialcalculated by the pseudopotential theory with various types of pseudopotentials. Very recently, we (Hoshino et af 1990a, 1990b, Mori et al 1990 have investigated the structure of expanded liquid Cs along the liquid-vapour coexistence curve by the integral equation theory in the modified hypernetted-chain (MHNC) approximation and by the molecular dynamics (m) simulation, and succeeded in reproducing the characteristic features of the structure of expanded liquid Cs observed by Winter eta1 (1987).…”

Dynamic structure of expanded liquid rubidium from a molecular-dynamics simulation

“…There are also theoretical and molecular-dynamics (MD) studies on the expanded liquid alkali metals with the effective pair potentials derived by means of the pseudopotential perturbation theory. Hoshino et al [8][9][10][11][12] studied the density dependence of both the static and the dynamic structures of expanded liquid alkali metals by using the integral equation theory and the viscoelastic approximation. The characteristic features of the observed density dependence of the structure are well reproduced from the triple point up to about three times the critical density.…”