Spin-density-functional theory is employed to calculate the conductance G t
hrough a quasi-one-dimensional quantum wire. In addition to the usual subba
nd quantization plateaus at G=n(2e(2)/h), we find additional structures at
(n+1/2)(2e(2)/h). The extra structures appear whether or not the electrons
in the wire spin polarize. However, only the spin-polarized case reproduces
the experimental temperature and magnetic field dependences.