S. Kammerer et al., TEST OF MODE-COUPLING THEORY FOR A SUPERCOOLED LIQUID OF DIATOMIC-MOLECULES - I - TRANSLATIONAL DEGREES OF FREEDOM, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics, 58(2), 1998, pp. 2131-2140
A molecular-dynamics simulation is performed for a supercooled liquid
of rigid diatomic molecules. The time-dependent self and collective de
nsity correlators of the molecular centers of mass are determined and
compared with the predictions of the ideal mode coupling theory (MCT)
for simple liquids. This is done in real as well as in momentum space.
One of the main results is the existence of a unique transition tempe
rature T-c, at which the dynamics crosses over from an ergodic to a qu
asinonergodic behavior. The value for T-c agrees within the error bars
with that found earlier for the orientational dynamics. In the first
scaling law regime of MCT, also called the beta regime, we find that t
he correlators in the late stage of the beta regime can be fitted well
by the von Schweidler law. Although we do not observe the critical de
cay predicted by MCT for the early beta-relaxation regime in its pure
form, our relaxation curves suggest that this decay is indeed present.
In this first scaling regime, a consistent description within ideal M
CT emerges only, if the next order correction to the asymptotic law is
taken into account. This correction is almost negligible for q = q(ma
x), the position of the main peak in the static structure factor S(q),
but becomes important for q = q(min), the position of its first minim
um. The second scaling law, i.e., the time-temperature superposition p
rinciple, holds reasonably well for the self and collective density co
rrelators and different values for q. The alpha-relaxation times tau(q
)((s)) and tau(q) follow a power law in T - T-c over two to three deca
des. The corresponding exponent gamma is practically q independent and
is around 2.55. This value is in agreement with the one predicted by
MCT from the value of the von Schweidler exponent but at variance with
the corresponding exponent gamma approximate to 1.6 obtained for the
orientational correlators C-1((s))(t) and C-1(t), studied in a previou
s paper.