We have derived an expression in terms of eigenvalues and eigenfunctio
ns of the no-pair Hamiltonian for the sum over the generalized oscilla
tor strength distribution for the relativistic, positive-energy soluti
ons for a many-electron system. Formally, it looks very much like the
corresponding nonrelativistic sum. However, only in the nonrelativisti
c limit is the sum equal to the number of electrons (the Bethe sum rul
e). We have determined the leading (1/c(2)) relativistic correction to
the nonrelativistic Bethe sum rule and we argue that this correction
is more in accordance with relativistic quantum mechanics than is a pr
evious suggestion. The same statement holds for relativistic correctio
ns to the Thomas-Reiche-Kuhn sum rule, previously derived only for one
-electron systems. We discuss the problem that the explicit summation
of the generalized oscillator strengths and calculation of the sum as
a groundstate average of a comutator, while formally equivalent, may n
ot give identical results in approximate calculations.