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A simple one dimensional glassy Kac model

Andrea Montanari1 and Antoine Sinton2

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We define a new family of random spin models with one-dimensional structure, finite-range multispin interactions, and bounded average degree (number of interactions in which each spin participates). Unfrustrated ground states can be described as solutions of a sparse, band diagonal linear system, thus allowing for efficient numerical analysis.

In the limit of infinite interaction range, we recover the so-called XORSAT (diluted p-spin) model that is known to undergo a random first-order phase transition as the average degree is increased. Here we investigate the most important consequences of a large but finite interaction range: (i) fluctuation-induced corrections to thermodynamic quantities; (ii) the need of an inhomogeneous (position-dependent) order parameter; (iii) the emergence of a finite mosaic length scale. In particular, we study the correlation length divergence at the (mean field) glass transition.


Keywords

structural glasses (theory)

disordered systems (theory)

exact results

 

E-print Number: 0705.0054

Cited: by |

Refers: to

PACS

75.10.Nr Spin-glass and other random models

64.70.P- Glass transitions of specific systems

65.60.+a Thermal properties of amorphous solids and glasses: heat capacity, thermal expansion, etc.

MSC

82C26 Dynamic and nonequilibrium phase transitions (general)

82C44 Dynamics of disordered systems (random Ising systems, etc.)

82C80 Numerical methods (Monte Carlo, series resummation, etc.)

82C35 Irreversible thermodynamics, including Onsager-Machlup theory

Subjects

Condensed matter: electrical, magnetic and optical

Condensed matter: structural, mechanical & thermal

Dates

Issue 08 (August 2007)

Received 7 May 2007, accepted for publication 11 June 2007

Published 1 August 2007



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