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  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Communications in mathematical physics 135 (1991), S. 483-497 
    ISSN: 1432-0916
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics , Physics
    Notes: Abstract Let $$\left\{ {J_{\left\langle {x,y} \right\rangle } } \right\}_{\left\langle {x,y} \right\rangle \subset Z^d } $$ and $$\left\{ {K_x } \right\}_{x \in Z^d } $$ be independent sets of nonnegative i.i.d.r.v.'s, 〈x,y〉 denoting a pair of nearest neighbors inZ d; let β, γ〉0. We consider the random systems: 1. A bond Bernoulli percolation model onZ d+1 with random occupation probabilities 2. Ferromagnetic random Ising-Potts models onZ d+1; in the Ising case the Hamiltonian is $$H = - \beta \sum\limits_t {\sum\limits_{\left\langle {x,y} \right\rangle } {J_{\left\langle {x,y} \right\rangle } \sigma (x,t)\sigma (y,t) - } \gamma \sum\limits_x {\sum\limits_t {K_x \sigma (x,t)} \sigma (x,t + 1)} } $$ For such (d+1)-dimensional systems withd-dimensional disorder we prove: (i) for anyd≧1, if β and γ are small, then, with probability one, the two-point functions decay exponentially in thed-dimensional distance and faster than polynomially in the remaining dimension, (ii) ifd≧2, then, with probability one, we have long-range order for either and β with γ sufficiently large of β sufficiently large and any γ.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    Communications in mathematical physics 135 (1991), S. 499-515 
    ISSN: 1432-0916
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics , Physics
    Notes: Abstract We study the zero-temperature behavior of the Ising model in the presence of a random transverse field. The Hamiltonian is given by $$H = - J\sum\limits_{\left\langle {x,y} \right\rangle } {\sigma _3 (x)\sigma _3 (y) - \sum\limits_x {h(x)\sigma _1 (x)} } $$ whereJ〉0,x,y∈Z d, σ1, σ3 are the usual Pauli spin 1/2 matrices, andh={h(x),x∈Z d} are independent identically distributed random variables. We consider the ground state correlation function 〈σ3(x)σ3(y)〉 and prove: 1. Letd be arbitrary. For anym〉0 andJ sufficiently small we have, for almost every choice of the random transverse fieldh and everyx∈Z d, that $$\left\langle {\sigma _3 (x)\sigma _3 (y)} \right\rangle \leqq C_{x,h} e^{ - m\left| {x - y} \right|} $$ for ally∈Z d withC x h 〈∞. 2. Letd≧2. IfJ is sufficiently large, then, for almost every choice of the random transverse fieldh, the model exhibits long range order, i.e., $$\mathop {\overline {\lim } }\limits_{\left| y \right| \to \infty } \left\langle {\sigma _3 (x)\sigma _3 (y)} \right\rangle 〉 0$$ for anyx∈Z d.
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  • 3
    Electronic Resource
    Electronic Resource
    Springer
    Communications in mathematical physics 104 (1986), S. 227-241 
    ISSN: 1432-0916
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics , Physics
    Notes: Abstract LetH=−Δ+V onl 2(ℤ), whereV(x),x∈ℤ, are i.i.d.r.v.'s with common probability distributionv. Leth(t)=∫e −itv dv(v) and letk(E) be the integrated density of states. It is proven: (i) Ifh isn-times differentiable withh (j)(t)=O((1+|t|)−α) for some α〉0,j=0, 1, ...,n, thenk(E) is aC n function. In particular, ifv has compact support andh(t)=O((1+|t|)−α) with α〉0, thenk(E) isC ∞. This allowsv to be singular continuous. (ii) Ifh(t)=O(e −α|t|) for some α〉0 thenk(E) is analytic in a strip about the real axis. The proof uses the supersymmetric replica trick to rewrite the averaged Green's function as a two-point function of a one-dimensional supersymmetric field theory which is studied by the transfer matrix method.
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  • 4
    Electronic Resource
    Electronic Resource
    Springer
    Communications in mathematical physics 74 (1980), S. 15-20 
    ISSN: 1432-0916
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics , Physics
    Notes: Abstract In the first part of this note we find conditions under which the frequency spectrum of a transformation exhibits delta functions. In the second part we show that if an ergodic flow on anm-dimensional manifold hasm−1 strictly negative characteristic exponents, then the measure is concentrated either on a fixed point or on a closed attracting orbit.
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  • 5
    Electronic Resource
    Electronic Resource
    Springer
    Communications in mathematical physics 130 (1990), S. 441-456 
    ISSN: 1432-0916
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics , Physics
    Notes: Abstract We show that at the special energiesE=2cosπp/q, the invariant measure, the Lyapunov exponent, and the density of states can be extended to zero disorder as C∞ functions in the disorder parameter. In particular, we obtain asymptotic series in the disorder parameter. This gives a rigorous proof of the existence of the anomalies originally discovered by Kappus and Wegner and studied by Derrida and Gardner and by Bovier and Klein.
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  • 6
    Electronic Resource
    Electronic Resource
    Springer
    Communications in mathematical physics 114 (1988), S. 439-461 
    ISSN: 1432-0916
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics , Physics
    Notes: Abstract We prove smoothness of the density of states in the Anderson model at high disorder for a class of potential distributions that include the uniform distribution.
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  • 7
    Electronic Resource
    Electronic Resource
    Springer
    Communications in mathematical physics 124 (1989), S. 543-552 
    ISSN: 1432-0916
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics , Physics
    Notes: Abstract We prove that the density of states for the tight-binding model with off-diagonal disorder under general conditions diverges forR→0 at least as $$ \sim \frac{1}{{\left| E \right|(\ln \left| E \right|)^4 }}$$ . This result is established through the study of the recurrence properties of an associated Markov chain.
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  • 8
    Electronic Resource
    Electronic Resource
    Springer
    Probability theory and related fields 88 (1991), S. 269-341 
    ISSN: 1432-2064
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics
    Notes: Summary We consider thed-dimensional Bernoulli bond percolation model and prove the following results for allp〈p c : (1) The leading power-law correction to exponential decay of the connectivity function between the origin and the point (L, 0, ..., 0) isL −(d−1)/2 . (2) The correlation length, ξ(p) is real analytic. (3) Conditioned on the existence of a path between the origin and the point (L, 0, ..., 0), the hitting distribution of the cluster in the intermediate planes,x 1 =qL,0〈q〈1, obeys a multidimensional local limit theorem. Furthermore, for the two-dimensional percolation system, we prove the absence of a roughening transition: For allp〉p c , the finite-volume conditional measures, defined by requiring the existence of a dual path between opposing faces of the boundary, converge—in the infinite-volume limit—to the standard Bernoulli measure.
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  • 9
    Electronic Resource
    Electronic Resource
    Springer
    Journal of statistical physics 54 (1989), S. 81-88 
    ISSN: 1572-9613
    Keywords: Disordered systems ; Gibbs states ; symmetry breaking
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract We prove that Gibbs states for the Hamiltonian $$H = - \sum\nolimits_{xy} {\tilde J_{xy} s_x \cdot s_y } $$ , with thes x varying on theN-dimensional unit sphere, obtained with nonrandom boundary conditions (in a suitable sense), are almost surely rotationally invariant if $$\tilde J_{xy} = {{J_{xy} } \mathord{\left/ {\vphantom {{J_{xy} } {\left| {x - y} \right|^\alpha }}} \right. \kern-\nulldelimiterspace} {\left| {x - y} \right|^\alpha }}$$ withJ xy i.i.d. bounded random variables with zero average, α⩾ 1 in one dimension, and α⩾2 in two dimensions.
    Type of Medium: Electronic Resource
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  • 10
    Publication Date: 1991-09-01
    Print ISSN: 0178-8051
    Electronic ISSN: 1432-2064
    Topics: Mathematics
    Published by Springer
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