On a classical spin glass model
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Mydosh, J.A.: In: Springer Lecture Notes in Physics. Vol. 149, p. 87. Berlin, Heidelberg, New York: Springer 1981
Monod, P., Bouchiat, H.: In: Springer Lecture Notes in Physics. Vol. 149, p. 118. Berlin, Heidelberg, New York: Springer 1981; J. Phys. (Paris)43, L45 (1982)
Morgownik, A.F.J., Mydosh, J.A.: Physica107B, 305 (1981); Phys. Rev. B24, 5277 (1981)
Penrose, O., Lebowitz, J.L.: In: Fluctuation phenomena. Montroll, E.W., Lebowitz, J.L. (eds), Chap. 5. Amsterdam: North-Holland 1979
Sommers, H.J.: Z. Phys. B-Condensed Matter31, 301 (1978);33, 173 (1979)
Gabay, M.: Ph.D. Thesis, Orsay 1981
For a review see G. Toulouse, ?Frustrations et désordres: problèmes nouveaux en mécanique statistique. Histoire des verres de spin?, Meeting, Clermont-Ferrand (1981) J. Phys. (Paris) (to be published)
Toulouse, G.: Commun. Phys.2, 115 (1977)
Springer, M.D.: The algebra of random variables. New York: Wiley 1979
Lamperti, J.: Probability. Sect. 14. New York: Benjamin 1966
Huang, K.: Statistical mechanics. Sect. 8.2. New York: Wiley 1963
Bruijn, N.G. de: Asymptotic methods in analysis. 2nd Edn., Sect. 4.2. Amsterdam: North-Holland 1961
Using the strong law of large numbers (Ref. 23, Sect. 7) or the ergodic theorem
Cramér, H.: Act. Sci. Ind., Vol. 736, pp. 5?23. Paris: Hermann 1938
Roberts, A.W., Varberg, D.E.: Convex functions, pp. 30 and 110. New York: Academic Press 1973
Kac, M.: In: Statistical physics, phase transitions and superfluidity. Chrétien, M., Gross, E.P., Deser, S. (eds.), Vol. 1, pp. 248?249. New York: Gordon and Breach 1968. See also Stanley, H.E.: Introduction to phase transitions and critical phenomena. Sect. 6.5. Oxford: Oxford University Press 1971
Donsker, M.D., Varadhan, S.R.S.: Phys. Rep.77, 235 (1981) and references quoted therein. Additional information may be found in Ref.32. See also R.S. Ellis, Large deviations and other limit theorems for a class of dependent random variables with applications to statistical mechanics, Z. Wahrscheinlichkeitstheorie (submitted for publication)
Ref. 22, Sect. 15
If one scales by 1/2N instead ofN and replacesK by ?J 0 one just gets (3.13). Hence the transition atK=1; it is second order
Scaling by 1/2N instead ofN in theJ 0-term leaves us with an extra factor 1/2 so that the ferromagnetic transition itself would occur at 1/2?J 0=1. Note this transition is second order too
Landau, L.D., Lifshitz, E.M.: Statistical physics. 2nd. Edn., pp. 478?479. Oxford: Pergamon Press 1969
Ref. 31, Theorem 15.D and problem 43.D
Eisele, Th., Ellis, R.S.: Symmetry breaking and random waves for magnetic systems on a circle. Preprint, Heidelberg, 1981, Appendix C
See also a recent discussion in Phys. Rev. Lett.: Gullikson, E.M., Schultz, S.: Phys. Rev. Lett.49, 238 (1982)
Ref. 31??, 110, and 115 New York: Academic Press 1973
Ref. 31?? and Theorem 51.E New York: Academic Press 1973
Chung, K.L.: Elementary probability theory with stochastic processes. 2nd Edn., Sect. 7.3. Berlin, Heidelberg, New York: Springer-Verlag 1975
Feller, W.: An introduction to probability theory and its applications. Vol. I, 3rd Edn., Sect. VII.3. New York: Wiley 1970
Ref. 31??, Theorem 42.F New York: Academic Press 1973
Iooss, G., Joseph, D.D.: Elementary stability and bifurcation theory. Berlin, Heidelberg, New York: Springer-Verlag 1980
Eisele, Th., Enter, A.C.D. van, Hemmen, J.L. van: (Manuscript in preparation)
See, for instance, Verbeek, B.H., Nieuwenhuys, G.J., Stocker, H., Mydosh, J.A.: Phys. Rev. Lett.40, 586 (1978)
See also Joffrin, J.: In: Ill-condensed matter, Les Houches 1978. Balian, R., Maynard, R., Toulouse, G. (eds.), Sects. 1.1 and 1.2. Amsterdam: North-Holland 1979
Binder, K.: In: Fundamental problems in statistical mechanics. Cohen, E.G.D. (ed.), Vol. V, pp. 21?51. Amsterdam: North-Holland 1980
