Abstract
The (d=2)-dimensional spin model composed of alternating strips of two different Ising magnets is revisited. Application of modern techniques results in explicit exact solution for the free energy and correlation lengths of the continuous (field-theoretic) limit of the model. In agreement with earlier results, the specific heat generally exhibitsthree different critical features: two near the respective critical temperaturesT c1 andT c2 of the composing models, as well as a new superlattice transition atT c1 <T c <T c2 . Further analysis shows that at all temperatures betweenT c1 andT c2 the correlations in the system include a low-amplitude but very long-range component reflecting fluctuations in a largescale domain wall network. The essential features of the solution can be explained by a reentrant dimensional crossover from thed=2, bulk behavior within the strips, to one-dimensional criticality in the individual strips, and finally back to the two-dimensional behavior on a new, superlattice level. This qualitative understanding of the physical content of the model allows for semiquantitative description of the temperature dependence of spontaneous magnetization and magnetic susceptibility, which have been previously obscure.
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References
L. Onsager,Phys. Rev. 65:117 (1944).
B. M. McCoy and T. T. Wu,The Two-Dimensional Ising Model (Harvard University Press, Cambridge, Massachusetts, 1973).
M. E. Fisher and A. E. Ferdinand,Phys. Rev. Lett. 19:169 (1967); A. E. Ferdinand and M. E. Fisher,Phys. Rev. 185:832 (1969).
H. Au-Yang and M. E. Fisher,Phys. Rev. B 21:3956 (1980), and references therein.
K. Binder and P. C. Hohenberg,Phys. Rev. B 6:3461 (1972).
D. S. Fisher,Phys. Rev. Lett. 69:534 (1992).
M. E. Fisher,J. Phys. Soc. Suppl. 26:87 (1969); A. E. Ferdinand and M. E. Fisher, Unpublished.
F. Becker and H. Hahn,Phys. Lett. 42A:9 (1972); I. Decker and H. Hahn,Physica 83A:143 (1976);89A:37 (1977);93A:215 (1978).
C. F. Majkrzak et al.,Adv. Phys. 40:99 (1991).
A. P. Y. Wong, S. B. Kim, W. I. Goldburg, and M. H. W. Chan,Phys. Rev. Lett. 70:954 (1993), and references therein.
L. V. Mikheev and M. E. Fisher,J. Stat. Phys. 66:1225 (1992).
L. V. Mikheev and M. E. Fisher,Phys. Rev. Lett. 70:186 (1993).
L. V. Mikheev and M. E. Fisher,Phys. Rev. B 49 (1994).
J. K. Percus,J. Stat. Phys. 60:221 (1990).
R. Shankar and G. Murthy,Phys. Rev. B 36:536 (1987).
L. V. Mikheev, in preparation.
R. Lipowsky and M. E. Fisher,Phys. Rev. B 36:2126 (1987), and references therein.
M. E. Fisher,J. Stat. Phys. 34:667 (1984), Section 11.
V. Privman and M. E. Fisher,J. Stat. Phys. 33:385 (1983).
L. D. Landau and E. M. Lifshitz,Statistical Physics (Pergamon Press, New York, 1980), §163.
A. Z. Patashinskii and V. L. Pokrovskii,Fluctuation Theory of Phase Transitions (Pergamon Press, New York, 1979).
L. V. Mikheev, in preparation.
M. E. Fisher, inCollective Properties of Physical Systems, B. Lundqvist and S. Lundqvist, eds. (Academic Press, New York, 1973).
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Mikheev, L.V. Reentrant dimensional crossover in planar Ising superlattices. J Stat Phys 78, 79–101 (1995). https://doi.org/10.1007/BF02183339
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DOI: https://doi.org/10.1007/BF02183339