Abstract
We map the Edwards Anderson Hamiltonian onto an effective Hamiltonian for Ising spins with nonrandom competing couplings. A high-temperature series is used to calculate the coupling constants to 20th, 16th, and 12th order for two, three, and four dimensions, respectively. We conclude the lower critical dimension to be close to three and find the correlation-length and susceptibility critical exponents to be twice as large as for thed=3 Ising model.
Similar content being viewed by others
References
Sherrington, D., Kirkpatrick, S.: Phys. Rev. Lett.32, 1792 (1975)
Edwards, S.F., Anderson, P.W.: J. Phys. F5, 965 (1975)
Ogielski, A.T., Morgenstern, I.: Phys. Rev. Lett.54, 928 (1985);
Ogielski, A.T.: Phys. Rev. B32, 7384 (1985)
Singh, R.R.P., Chakravarty, S.: Phys. Rev. Lett.57, 245 (1986)
Bhatt, R.N., Young, A.P.: Phys. Rev. Lett.54, 924 (1985); Mc Millan, W.L.: Phys. Rev. B31, 340 (1985); Bray, A.J., Moore, M.A.: Phys. Rev. B31, 631 (1985)
Moore, A.M., Bray, A.J.: J. Phys. C18, L699 (1985); Moore, A.M.: J. Phys. A19, L211 (1986); see also references cited in Hemmen, J.L. van: J. Phys. C19, L379 (1986)
Haake, F., Lewenstein, M., Wilkens, M.: Phys. Rev. Lett.55, 2606 (1985)
Fischer, K.H.: Phys. Status Solidi (b)116, 357 (1983)
Baxter, R.J.P.: Phys. Rev. Lett.26, 832 (1971); Wu, F.W.: Phys. Rev. B4, 2312 (1971). In fact the eight vertex model is solvable exactly forK 1=0,K 2≠0,K □≠0 ind=2. Approximate results forK 1≠0 ind=2 are given in Nauenberg, M., Nienhuis, B.: Phys. Rev. Lett.33, 944 (1974); Leeuwen, J.M.J. van: Phys. Rev. Lett.34, 1056 (1975); Nightingale, M.P.: Phys. Lett. A59, 486 (1976)
Any coupling ofm spins is of orderK 2n, wheren is the minimal number of nearest-neighbor-steps which connect thesem spins in a closed loop
Griffiths, H.P., Wood, D.W.: J. Phys. C7, 4021 (1974); Gitterman, M., Mikulinsky, M.: J. Phys. C10, 4073 (1977)
Haake, F., Lewenstein, M., Wilkens, M.: Z. Phys. B54, 333 (1984)
Baker, G.A., Groves-Morris, P.: Padé approximants. Part I. Encyclopedia of mathematics and it's applications. Amsterdam: Addison-Wesley Publ. 1981
This indicates a pole on the negative χ (or ξ) axis close to the origin which dominates the series under consideration
Wilkens, M.: Dissertation (unpublished)
Domb, C., Green, M.S. (eds.): Phase transitions and critical phenomena. Vol. 3. New York: Academic Press
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Haake, F., Lewenstein, M. & Wilkens, M. Equivalence of random and competing nonrandom bonds for Edwards Anderson spin-glass. Z. Physik B - Condensed Matter 66, 201–209 (1987). https://doi.org/10.1007/BF01311656
Received:
Issue Date:
DOI: https://doi.org/10.1007/BF01311656