Martynov Sarkisov Vompe

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The Martynov-Sarkisov-Vompe (MSV) (Eq. 33 of [1]) closure relation is given in terms of the bridge function:

B^{(2)}(r) = - \frac{1}{2} (\omega - \phi)^2

where

\left.\phi\right. =  \rho \epsilon \beta

where \phi is short-ranged. The Weeks-Chandler-Andersen division of the Lennard-Jones potential was used. (Notice that the Martynov-Sarkisov-Vompe closure, for a hard sphere fluid, becomes the Martynov Sarkisov closure).

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