Abstract

The localization properties of certain spin-dependent, one-dimensional electronic systems with only off-diagonal disorder are studied. In higher dimensions (d=2,3) the models considered would correspond to different universality classes, whereas ford=1 no qualitative difference is found: ForE=0, all eigenstates are exponentially localized, whereas forE→0 the localization length diverges logarithmically, such that exactly atE=0 the geometric average of the transmission coefficient would decay with increasing chain lengthL as exp (-const. ·L 1/2), instead of the usual, exponential decay. ForE=0, in the interior of the band, the localization lengthr 0 diverges ∼W 2 −2 in the limit of weak disorder (W 2→0), whereas just at the band edge one has roughlyr 0∼W 2 −2/3. A universal recursion relation, depending only on the energy and on certain randomly distributed determinants, determines the localization length and the density of states for all systems considered.

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