1987
DOI: 10.1051/jphys:01987004805071300
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On classical spin-glass models

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Cited by 11 publications
(5 citation statements)
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“…We have shown that the distribution of spin-spin interaction constants can be found directly by way of calculations of classical Equations (5) and analysis of statistical data of simulation. It is theoretically shown (see inequality (16)) that at least for the 1D spin-glass problem the distribution of the spin-spin interaction constants can not be Gauss-Edwards-Anderson type. In particular, the analysis of numerical data of simulation shows that they obey to Lévys alpha-stable distribution law.…”
Section: Discussionmentioning
confidence: 99%
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“…We have shown that the distribution of spin-spin interaction constants can be found directly by way of calculations of classical Equations (5) and analysis of statistical data of simulation. It is theoretically shown (see inequality (16)) that at least for the 1D spin-glass problem the distribution of the spin-spin interaction constants can not be Gauss-Edwards-Anderson type. In particular, the analysis of numerical data of simulation shows that they obey to Lévys alpha-stable distribution law.…”
Section: Discussionmentioning
confidence: 99%
“…The algorithm works as follows. Randomly M sets of initial parameters are generated and parallel calculations of Equation (17) for unknown variables i x and i y transact taking into account conditions (16) and (18). However only specifying initial conditions is not enough for the solution of these equations.…”
Section: Numerical Experimentsmentioning
confidence: 99%
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“…In the models of second type the bond-randomness is expressed in terms of some underlining hidden site-randomness and is thus of a superficial nature. It has been pointed out in the works [14][15][16], however, this feature retains an important physical aspect of true spin glasses, viz. they are random with respect to the positions of magnetic impurities.…”
Section: Introductionmentioning
confidence: 97%
“…The case where M is is strictly bounded could be termed "standard disordered mean field", and it is this type of models that were studied by Pastur and Figotin in 1977, the case of two patterns having been introduced by Luttinger [Lut] shortly before that. Such "site-disorder" models were studied again intensely some years later by a number of people, emphasizing applications of large deviation methods [vHvEC,vH1,GK,vHGHK,vH2,AGS2,JK,vEvHP]. A general large deviation theory for such systems was obtained by Comets [Co] somewhat later.…”
Section: Introductionmentioning
confidence: 99%