We apply dimensional perturbation theory to the calculation of Regge p
ole positions, providing a systematic improvement to earlier analytic
first-order results. We consider the orbital angular momentum l as a f
unction of spatial dimension D for a given energy E, and expand l in i
nverse powers of kappa=(D-1)/2. It is demonstrated for both bound and
resonance states that the resulting perturbation series often converge
s quite rapidly, so that accurate quantum results can be obtained via
simple analytic expressions given here through third order. For the qu
artic oscillator potential, the rapid convergence of the present l(D;E
) series is in marked contrast with the divergence of the more traditi
onal E(D;l) dimensional perturbation series, thus offering an attracti
ve alternative for bound state problems. (C) 1997 American Institute o
f Physics.