Measuring the fluctuation-dissipation ratio in glassy systems with no perturbing field

Physical Review E - Statistical, Nonlinear, and Soft Matter Physics

Volumn 68, Issue 6 2, 2003, Pages 651041-651044

  Ricci Tersenghi, F ^a  

^a UNIVERSITÀ DI ROMA LA SAPIENZA   (Italy)

Author keywords

[No Author keywords available]

Indexed keywords

COMPUTATIONAL COMPLEXITY; COMPUTER SIMULATION; GLASS; HAMILTONIANS; MATHEMATICAL MODELS; MONTE CARLO METHODS; POLYMERS; RANDOM PROCESSES; SIGNAL TO NOISE RATIO; THERMODYNAMICS;

BIOMOLECULES; FLUCTUATION-DISSIPATION RATIO (FDR); GLASS-FORMER LIQUIDS; GLASSY SYSTEMS; PERTURBING FIELDS;

PHASE TRANSITIONS;

EID: 1442281484     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: None     Document Type: Article

References (17)

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2. For review see J.-P. Bouchaud et al., in Spin Glasses and Random Fields, edited by A. P. Young (World Scientific, Singapore, 1997); L.F. Cugliandolo, e-print cond-mat/0210312.
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7. t→∞C(t,s) = 0 ∀ s<∞, and normalized, C(t,t) = 1.
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12. Accelerated dynamics can be used only in some particularly simple cases.
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14. In the first version of Ref. [10], the only one available at the time this work was finished, only the punctual response function R(t,s) was studied and the calculations had some errors, making the final result unreliable.
15. F. Krzakala and F. Ricci-Tersenghi (unpublished).
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