The effects due to electron scattering by rough boundaries on the electrica
l conductivity of quantum wires are analysed theoretically in the diffusive
regime. The boundary roughness is assumed to be random self-affine fractal
characterised by the roughness exponent H, roughness correlation length xi
, and rms roughness amplitude Delta. In the limit of small correlation leng
ths and a single occupied quasi-one-dimensional miniband, the conductivity
a shows sigma power-law behaviour with the wire width d, sigma proportional
to d(9). For large N, on the other hand, the conductivity increases then a
s sigma proportional to d(c) (c approximate to 2) with increasing d.