Martynov Sarkisov Vompe

The Martynov-Sarkisov-Vompe (MSV) (1999) (Eq. 33 Ref. 1) closure 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 WCA division of the LJ potential was used. (Notice that the MSV closure, for a hard sphere fluid, becomes the MS closure).

References

1. [JCP_1999_110_03961]