We study a model of a stripe ordered doped antiferromagnet consisting of
coupled Hubbard ladders which can be tuned from quasi-one-dimensional to
two-dimensional. We solve for the magnetization and charge density on the
ladders by Hartree-Fock theory and find a set of solutions with lightly doped
spin-stripes'' which are antiferromagnetic and more heavily doped anti-phase charge-stripes’‘. Both the spin- and charge-stripes have electronic spectral
weight near the Fermi energy but in different regions of the Brillouin zone;
the spin-stripes in the nodal'' region, near (\pi/2,\pi/2), and the charge-stripes in the antinodal’’ region, near (\pi,0). We find a striking
dichotomy between nodal and antinodal states in which the nodal states are
essentially delocalized and two-dimensional whereas the antinodal states are
quasi-one-dimensional, localized on individual charge-stripes. For
bond-centered stripes we also find an even-odd effect of the charge periodicity
which could explain the non-monotonous variations with doping of the
low-temperature resistivity in LSCO

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