Analytic bond-order potentials (BOP's) are derived for the sigma and pi bon
d orders by approximating the many-atom expansion for the bond order within
the two-center, orthogonal tight-binding (TB) model. The analytic expressi
on, BOP4, is obtained by retaining terms to four levels in the continued fr
actions for the appropriate Green's functions and describes the sigma bonds
in the dimer C-2, the tetrahedral methane molecule CH4 and the trigonal me
thyl radical CH3 exactly. A simplified, but accurate, variant, BOP4S, depen
ds only on the two recursion coefficients b(1) and b(2) that characterize t
he root-mean-square width and the unimodal versus bimodal shape of the sigm
a bond eigenspectrum, respectively. An analytic expression for the pi bond
order, BOP2M, is obtained by performing matrix recursion to two levels, the
reby ensuring that the expression is independent of the choice of coordinat
e axes, depending only on neighboring bond integrals, bund angles and dihed
ral angles. A simple analytic expression for the promotion energy is also p
resented. Advantages of these BOP's over the empirical Tersoff-Brenner pote
ntials are, first, their analytic form is predicted by the theory, second,
the sigma bond order expression BOP4S includes the very important shape par
ameter (b(2)/b(1))(2), and third, the pi bond order expression BOP2M descri
bes the breaking of saturated pi bonds both on radical formation and under
torsion. The following paper examines the accuracy of these BOP's for model
ing the energetics of diamond, graphite, and hydrocarbon molecules. [S0163-
1829(99)03313-5].