The total number of ground states for short-range Ising spin glasses, defin
ed on diamond hierarchical lattices of fractal dimensions d=2, 3, 4, 5, and
2.58, is estimated by means of analytic calculations (three last hierarchy
levels of the d=2 lattice) and numerical simulations (lower hierarchies fo
r d=2 and all remaining cases). It is shown that in the case of continuous
probability distributions for the couplings, the number of ground states is
finite in the thermodynamic limit. However, for a bimodal probability dist
ribution (+/-J with probabilities p and 1-p, respectively), the average num
ber of ground slates is maximum for a wide range of values of p around p =
1/2 and depends on the total number of sites at hierarchy level n, N-(n). I
n this case, for all lattices investigated, it is shown that the ground-sta
te degeneracy behaves like exp[h(d)N-(n)], in the limit N-(n) large, where
h(d) is a positive number which depends on the lattice fractal dimension. T
he probability of finding frustrated cells at a given hierarchy level n, F-
(n)(p), is calculated analytically (three last hierarchy levels for d=2 and
the last hierarchy of the d=3 lattice, with 0 less than or equal to p less
than or equal to 1), as well as numerically (all other cases, with p = 1/2
). Except for d=2, in which case F-(n)(1/2) increases by decreasing the hie
rarchy level, all other dimensions investigated present an exponential decr
ease in F-(n)(1/2) for decreasing values of n. For d=2 our results refer to
the paramagnetic phase, whereas for all other dimensions considered [which
are greater than the lower critical dimension d(l) (d(l) approximate to 2.
5)], our results refer to the spin-glass phase at zero temperature; in the
latter cases h(d) increases with the fractal dimension. For n much greater
than 1, only the last hierarchies contribute significantly to the ground-st
ate degeneracy; such a dominant behavior becomes stronger for high fractal
dimensions. The exponential increase of the number of ground states with th
e total number of sites is in agreement with the mean-field picture of spin
glasses. [S1063-651X(99)07910-6].