The chaotic renormalization‐group trajectories exhibited by frustrated hierarchical Ising models have been interpreted as signaling a spin‐glass phase, since, as the system is probed at successive length scales, strong and weak correlations are encountered in a chaotic sequence. Cluster‐hierarchical models have been introduced, with susceptibilities behaving as in Bravais lattices. Frustrated cluster‐hierarchical models again show an ordered phase characterized by chaotic rescaling and a smooth specific heat at the transition (α<−5). Scans in dimensionality reveal an upper critical dimension for the chaotic spin‐glass phase, via a boundary crisis mechanism. Beyond this dimension, the system has no long‐range order at any temperature. Nevertheless, a low‐temperature regime can be distinctly identified, exhibiting intermediate‐range chaotic spin‐glass order.
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15 March 1984
Research Article|
March 15 1984
Chaotic spin glasses: An upper critical dimension (invited)
Susan R. McKay;
Susan R. McKay
Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139
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A. Nihat Berker
A. Nihat Berker
Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139
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J. Appl. Phys. 55, 1646–1648 (1984)
Citation
Susan R. McKay, A. Nihat Berker; Chaotic spin glasses: An upper critical dimension (invited). J. Appl. Phys. 15 March 1984; 55 (6): 1646–1648. https://doi.org/10.1063/1.333429
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