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Thermodynamical Limit for Correlated Gaussian Random Energy Models
"... Let fE (N)g 2N be a family of j N j = 2 random variables de ned by the covariance matrix CN of elements c N (; ) := Av (E (N)E (N)), and HN () = NE (N) the corresponding random Hamiltonian. Then the quenched thermodynamical limit exists if, for every decomposition N = N 1 + N 2 , and a ..."
Abstract

Cited by 9 (3 self)
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Let fE (N)g 2N be a family of j N j = 2 random variables de ned by the covariance matrix CN of elements c N (; ) := Av (E (N)E (N)), and HN () = NE (N) the corresponding random Hamiltonian. Then the quenched thermodynamical limit exists if, for every decomposition N = N 1 + N 2
Let {Eσ(N)}σ∈ΣN
, 2002
"... be a family of ΣN  = 2 N centered unit Gaussian random variables defined by the covariance matrix CN of elements cN(σ,τ): = Av(Eσ(N)Eτ(N)), and HN(σ) = − √ NEσ(N) the corresponding random Hamiltonian. Then the quenched thermodynamical limit exists if, for every decomposition N = N1 + N2, and a ..."
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be a family of ΣN  = 2 N centered unit Gaussian random variables defined by the covariance matrix CN of elements cN(σ,τ): = Av(Eσ(N)Eτ(N)), and HN(σ) = − √ NEσ(N) the corresponding random Hamiltonian. Then the quenched thermodynamical limit exists if, for every decomposition N = N1 + N2
The Thermodynamic Limit in Mean Field Spin Glass Models
 Commun. Math. Phys
, 2002
"... We present a simple strategy in order to show the existence and uniqueness of the infinite volume limit of thermodynamic quantities, for a large class of mean field disordered models, as for example the SherringtonKirkpatrick model, and the Derrida pspin model. The main argument is based on a smoo ..."
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Cited by 116 (22 self)
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We present a simple strategy in order to show the existence and uniqueness of the infinite volume limit of thermodynamic quantities, for a large class of mean field disordered models, as for example the SherringtonKirkpatrick model, and the Derrida pspin model. The main argument is based on a
Jet quenching
, 902
"... Summary. We present a comprehensive review of the physics of hadron and jet production at large transverse momentum in highenergy nucleusnucleus collisions. Emphasis is put on experimental and theoretical “jet quenching ” observables that provide direct information on the (thermo)dynamical propert ..."
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Summary. We present a comprehensive review of the physics of hadron and jet production at large transverse momentum in highenergy nucleusnucleus collisions. Emphasis is put on experimental and theoretical “jet quenching ” observables that provide direct information on the (thermo)dynamical
Jet quenching
, 902
"... Summary. We present a comprehensive review of the physics of hadron and jet production at large transverse momentum in highenergy nucleusnucleus collisions. Emphasis is put on experimental and theoretical “jet quenching ” observables that provide direct information on the (thermo)dynamical propert ..."
Abstract
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Summary. We present a comprehensive review of the physics of hadron and jet production at large transverse momentum in highenergy nucleusnucleus collisions. Emphasis is put on experimental and theoretical “jet quenching ” observables that provide direct information on the (thermo)dynamical
Results 1  10
of
194,747