Strong Randomness Fixed Point in the Dissipative Random Transverse Field Ising Model

dc.creatorSchehr, Gregory
dc.creatorRieger, Heiko
dc.date2005-11-24
dc.date2006-04-20
dc.date.accessioned2026-07-07T06:49:24Z
dc.date.available2026-07-07T06:49:24Z
dc.descriptionThe interplay between disorder, quantum fluctuations and dissipation is studied in the random transverse Ising chain coupled to a dissipative Ohmic bath with a real space renormalization group. A typically very large length scale, L*, is identified above which the physics of frozen clusters dominates. Below L* a strong disorder fixed point determines scaling at a pseudo-critical point. In a Griffiths-McCoy region frozen clusters produce already a finite magnetization resulting in a classical low temperature behavior of the susceptibility and specific heat. These override the confluent singularities that are characterized by a continuously varying exponent z and are visible above a temperature T* ~ L*^{-z}.
dc.description4 pages RevTeX, figures included
dc.identifierhttps://arxiv.org/abs/cond-mat/0511608
dc.identifierhttp://arxiv.org/abs/cond-mat/0511608
dc.identifierPhys. Rev. Lett. 96, 227201 (2006)
dc.identifierdoi:10.1103/PhysRevLett.96.227201
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/104326
dc.subjectDisordered Systems and Neural Networks
dc.titleStrong Randomness Fixed Point in the Dissipative Random Transverse Field Ising Model
dc.typetext

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