2019
DOI: 10.1007/978-3-030-29077-1_3
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The Free Energy of the GREM with Random Magnetic Field

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Cited by 3 publications
(14 citation statements)
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“…3, is a generalization of Theorem 1.4 in [22], which addresses the case without a longitudinal field, h = 0. In the classical case without transversal magnetic field, b = 0, it generalizes the results of [7], which covers the case that h is constant, and of [4,5], which treats the special case of a REM or two-level GREM in a random magnetic field.…”
Section: The Quantum Grem With a Random Longitudinal Fieldmentioning
confidence: 59%
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“…3, is a generalization of Theorem 1.4 in [22], which addresses the case without a longitudinal field, h = 0. In the classical case without transversal magnetic field, b = 0, it generalizes the results of [7], which covers the case that h is constant, and of [4,5], which treats the special case of a REM or two-level GREM in a random magnetic field.…”
Section: The Quantum Grem With a Random Longitudinal Fieldmentioning
confidence: 59%
“…therein). Unlike for the SK-model, implementing the longitudinal field naively in GREM models causes the frozen phase to expand [4,5,7]. Derrida and Gardner [14] therefore suggested a hierarchical implementation of the longitudinal magnetic field, which then leads again to a destabilization of the frozen phase.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
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