We present the complete solution to the so-called ''Yukawa problem'' o
f the Skyrme model. This refers to the perceived difficulty of reprodu
cing, purely from soliton physics, the usual pseudovector pion-nucleon
coupling, echoed by pion coupling to the higher-spin/isospin baryons
(I=J=3/2,3/2,...,N-c/2) in a manner fixed by large-N-c group theory. T
he solution involves surprisingly elegant interplay between the classi
cal and quantum properties of a new configuration: the rotationally im
proved Skyrmion. This is the near-hedgehog solution obtained by minimi
zing the usual Skyrmion mass functional augmented by an all-important
(iso)rotational kinetic term. The numerics are pleasing: a Delta decay
width within a few MeV of its measured value, and, furthermore, the h
igher-spin baryons (I=J greater than or equal to 5/2) with widths so l
arge (Gamma > 800 MeV) that these undesirable large-N-c artifacts effe
ctively drop out of the spectrum, and pose no phenomenological problem
. Beyond these specific results, we ground the Skyrme model in the Fey
nman path integral, and set up a transparent collective coordinate for
malism that makes maximal use of the 1/N-c expansion. This approach el
ucidates the connection between Skyrmions on the one hand, and Feynman
diagrams in an effective held theory on the other.