We study at T=0 the minimum energy of a domain wall and its gap to the firs
t excited state, concentrating on two-dimensional random-bond Ising magnets
. The average gap scales as DeltaE(1)similar toL(theta)f(N-z), where f(y) s
imilar to [ln y](- 1/2), theta is the energy fluctuation exponent, L is the
length scale, and N-z is the number of energy valleys. The logarithmic sca
ling is due to extremal statistics, which is illustrated by mapping the pro
blem into the Kardar-Parisi-Zhang roughening process. It follows that the s
usceptibility of domain walls also has a logarithmic dependence on the syst
em size.