1994
DOI: 10.1088/0305-4470/27/23/008
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Block diagonalizing ultrametric matrices

Abstract: The problem of diagonalizing a class of complicated matrices, to be called ultrametric matrices, is investigated. These matrices appear at various stages in the description of disordered systems with many equilibrium phases by the technique of replica symmetry breaking. The residual symmetry, remaining after the breaking of permutation symmetry between replicas, allows us to bring all ultrametric matrices to a block diagonal form by a common similarity transformation. A large number of these blocks are, in fac… Show more

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Cited by 38 publications
(100 citation statements)
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References 16 publications
(37 reference statements)
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“…Fluctuations of the size of clusters, seem rather different in nature from the usual small fluctuations [56] of the amplitude of each element of the Parisi matrix. In particular in the case of REM the overlap between the states can be either 0 or 1 by the construction of the model so that fluctuation of the size of clusters amount to very large fluctuations of the amplitudes of the elements of the Parisi matrix [59].…”
Section: Appendix G: Fluctuations Of Clusters In One-step Rsb Solutionsmentioning
confidence: 78%
“…Fluctuations of the size of clusters, seem rather different in nature from the usual small fluctuations [56] of the amplitude of each element of the Parisi matrix. In particular in the case of REM the overlap between the states can be either 0 or 1 by the construction of the model so that fluctuation of the size of clusters amount to very large fluctuations of the amplitudes of the elements of the Parisi matrix [59].…”
Section: Appendix G: Fluctuations Of Clusters In One-step Rsb Solutionsmentioning
confidence: 78%
“…For a free-energy functional depending only on one order parameter matrix q aρ,bλ , the corresponding eigenvalues are Λ 011 and Λ 122 given by formula (41) in ref. [10]. In our case, however, the free-energy depends on 2K matrices {Q l ,Q l } and the stability condition for each mode reads ∆(α, K) =Λ ( Λ + (K − 1)Λ ) − 1 K 2 < 0 wherê Λ, Λ, Λ are the eigenvalues computed for the fluctuations with respect toQ ℓQℓ , Q ℓ Q ℓ and Q ℓ Q m (ℓ = m) respectively [2,4].…”
mentioning
confidence: 87%
“…Although it would require a complete analysis of the eigenvalues of the Hessian matrix, we have focused only on the replicons 011 and 122 in the notations of [10], which are usually the most "dangerous" modes [3]. For a free-energy functional depending only on one order parameter matrix q aρ,bλ , the corresponding eigenvalues are Λ 011 and Λ 122 given by formula (41) in ref.…”
mentioning
confidence: 99%
“…Within second-order variational perturbation theory, we obtain (H dis ) As before, we restrict ourselves to the transversal part of the 2 × 2 Green function G( Since G αβ is some matrix within the Parisi algebra the functional F has the ultrametric property [37,48]. Following Temesvári et al [48], we denote the size of the Parisi blocks with p r , r = 1 .…”
Section: Pure Disorder Terms In Hamiltonianmentioning
confidence: 99%