We have investigated liquid GeSe by first-principle molecular dynamics simu
lations performed in the framework of density functional theory. Our partia
l structure factors are in good agreement with recent experimental data. In
particular, we do not find any evidence of intermediate range order, as in
dicated by the absence of a first sharp diffraction peak for low magnitudes
of the momentum transfer in the partial structure factors. Comparison betw
een experimental and calculated partial pair correlation functions g(alpha
beta)(r) yields a less satisfactory agreement, non-negligible differences b
eing found particularly in the shape and peaks position of the g(GeGe)(r) a
nd g(SeSe)(r) for short distances (< 4 Angstrom). The origin of these discr
epancies are discussed in the light of recent experimental and theoretical
findings on other GexSe1-x disordered systems. Analysis of the atomic confi
gurations reveals that this liquid GeSe does not exhibit a regular network
structure. A variety of bonding configurations are found and, in particular
, the subunits GeSe3 and SeGe3 are frequently observed. A conspicuous amoun
t of Ge atoms form homopolar bonds, thereby favoring the occurrence of Ge-G
e-Se-3 groups in which the Ge-Ge bonds have a very short lifetime (similar
to 0.5 ps). However, neither these groups nor the GeSe3 and SeGe3 subunits
are predominant and play the role of the GeSe4 tetrahedra in the liquids Ge
Se4 and GeSe2, where structural order extended well beyond the first shell
of neighbors. The lack of a prevailing structural feature in liquid GeSe co
rrelates well with the absence of intermediate range order. (C) 2000 Americ
an Institute of Physics. [S0021- 9606(00)50437-1].