The effective Hamiltonian H-cap for a liquid-vapor interface is constructed
by using the "experimental" direct correlation function obtained from mole
cular-dynamics simulation. The density fluctuation is parametrized accordin
g to: (a) The standard shift of the density profile, parallel and small; (b
) the parallel shift; and (c) the shift with rotation as recently introduce
d, used in a density functional theory and compared with experiment. We fin
d a universal shape of H-cap, discussed in some detail. The shape strongly
suggests the existence of two regions of low wave-vector q and of high q co
rresponding to microscopic distances. Although bending and nonzero curvatur
e of the fluctuating interface are present, the apparent bending (rigidity)
coefficient is always negative, thus supporting the contention that the me
mbrane Hamiltonians are not applicable to normal liquid-vapor interfaces. S
everal definitions of the momentum-dependent surface tension are also discu
ssed. (C) 2001 American Institute of Physics.