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arXiv:2004.00064 · Physical review. B./Physical review. B

Beyond universal behavior in the one-dimensional chain with random nearest-neighbor hopping

Akshay Krishna, R. N. Bhatt

Published Jun 15, 2020• 10 citations
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Abstract

We study the one-dimensional nearest-neighbor tight-binding model of electrons with independently distributed random hopping and no on-site potential (i.e., off-diagonal disorder with particle-hole symmetry, leading to sublattice symmetry, for each realization). For nonsingular distributions of the hopping, it is known that the model exhibits a universal, singular behavior of the density of states $\ensuremath{\rho}(E)\ensuremath{\sim}1/|E{ln}^{3}|E||$ and of the localization length $\ensuremath{\xi}(E)\ensuremath{\sim}|ln|E||$, near the band center $E=0$. (This singular behavior is also applicable to random XY and Heisenberg spin chains; it was first obtained by Dyson for a specific random harmonic oscillator chain.) Simultaneously, the state at $E=0$ shows a universal, subexponential decay at large distances $\ensuremath{\sim}exp[\ensuremath{-}\sqrt{r/{r}_{0}}]$. In this study, we consider singular, but normalizable, distributions of hopping, whose behavior at small $t$ is of the form $\ensuremath{\sim}1/[t{ln}^{\ensuremath{\lambda}+1}(1/t)]$, characterized by a single, continuously tunable parameter $\ensuremath{\lambda}>0$. We find, using a combination of analytic and numerical methods, that while the universal result applies for $\ensuremath{\lambda}>2$, it no longer holds in the interval $0<\ensuremath{\lambda}<2$. In particular, we find that the form of the density of states singularity is enhanced (relative to the Dyson result) in a continuous manner depending on the nonuniversal parameter $\ensuremath{\lambda}$; simultaneously, the localization length shows a less divergent form at low energies and ceases to diverge below $\ensuremath{\lambda}=1$. For $\ensuremath{\lambda}<2$, the fall-off of the $E=0$ state at large distances also deviates from the universal result and is of the form $\ensuremath{\sim}exp[\ensuremath{-}{(r/{r}_{0})}^{1/\ensuremath{\lambda}}]$, which decays faster than an exponential for $\ensuremath{\lambda}<1$.

DOI
10.1103/physrevb.101.224203

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We study the one-dimensional nearest-neighbor tight-binding model of electrons with independently distributed random hopping and no on-site potential (i.e., off-diagonal disorder with particle-hole symmetry, leading to sublattice symmetry, for each realization). For nonsingular distributions of the hopping, it is known that the model exhibits a universal, singular behavior of the density of states \ensuremathρ(E)\ensuremath∼1/∣Eln3∣E∣∣\ensuremath{\rho}(E)\ensuremath{\sim}1/|E{ln}^{3}|E||\ensuremathρ(E)\ensuremath∼1/∣Eln3∣E∣∣ and of the localization length \ensuremathξ(E)\ensuremath∼∣ln∣E∣∣\ensuremath{\xi}(E)\ensuremath{\sim}|ln|E||\ensuremathξ(E)\ensuremath∼∣ln∣E∣∣, near the band center E=0E=0E=0. (This singular behavior is also applicable to random XY and Heisenberg spin chains; it was first obtained by Dyson for a specific random harmonic oscillator chain.) Simultaneously, the state at E=0E=0E=0 shows a universal, subexponential decay at large distances \ensuremath∼exp[\ensuremath−r/r0]\ensuremath{\sim}exp[\ensuremath{-}\sqrt{r/{r}_{0}}]\ensuremath∼exp[\ensuremath−r/r0​​]. In this study, we consider singular, but normalizable, distributions of hopping, whose behavior at small ttt is of the form \ensuremath∼1/[tln\ensuremathλ+1(1/t)]\ensuremath{\sim}1/[t{ln}^{\ensuremath{\lambda}+1}(1/t)]\ensuremath∼1/[tln\ensuremathλ+1(1/t)], characterized by a single, continuously tunable parameter \ensuremathλ>0\ensuremath{\lambda}>0\ensuremathλ>0. We find, using a combination of analytic and numerical methods, that while the universal result applies for \ensuremathλ>2\ensuremath{\lambda}>2\ensuremathλ>2, it no longer holds in the interval 0<\ensuremathλ<20<\ensuremath{\lambda}<20<\ensuremathλ<2. In particular, we find that the form of the density of states singularity is enhanced (relative to the Dyson result) in a continuous manner depending on the nonuniversal parameter \ensuremathλ\ensuremath{\lambda}\ensuremathλ; simultaneously, the localization length shows a less divergent form at low energies and ceases to diverge below \ensuremathλ=1\ensuremath{\lambda}=1\ensuremathλ=1. For \ensuremathλ<2\ensuremath{\lambda}<2\ensuremathλ<2, the fall-off of the E=0E=0E=0 state at large distances also deviates from the universal result and is of the form \ensuremath∼exp[\ensuremath−(r/r0)1/\ensuremathλ]\ensuremath{\sim}exp[\ensuremath{-}{(r/{r}_{0})}^{1/\ensuremath{\lambda}}]\ensuremath∼exp[\ensuremath−(r/r0​)1/\ensuremathλ], which decays faster than an exponential for \ensuremathλ<1\ensuremath{\lambda}<1\ensuremathλ<1.
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