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Volumn 63, Issue 1, 2001, Pages

Realistic spin glasses below eight dimensions: A highly disordered view

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EID: 18644370829     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.63.016101     Document Type: Article
Times cited : (10)

References (43)
  • 19
    • 85035253709 scopus 로고    scopus 로고
    • A completely rigorous proof, though, has so far been obtained only for (Formula presented)
    • A completely rigorous proof, though, has so far been obtained only for (Formula presented).
  • 21
    • 85035280067 scopus 로고    scopus 로고
    • This should not be confused with the milder phenomenon of chaotic temperature dependence 8 9, in which the pure states themselves change chaotically with temperature but their number does not
    • This should not be confused with the milder phenomenon of chaotic temperature dependence 89, in which the pure states themselves change chaotically with temperature but their number does not.
  • 27
  • 28
  • 32
    • 85035248182 scopus 로고    scopus 로고
    • Below four dimensions, quenched disorder is believed to result in domain wall wandering even at zero temperature. Domain wall wandering occurs also in uniform ferromagnets above the roughening temperature (which is zero in two dimensions and believed to be strictly below (Formula presented) in three dimensions), but for a different reason—resulting from thermal fluctuations, rather than from quenched disorder
    • Below four dimensions, quenched disorder is believed to result in domain wall wandering even at zero temperature. Domain wall wandering occurs also in uniform ferromagnets above the roughening temperature (which is zero in two dimensions and believed to be strictly below (Formula presented) in three dimensions), but for a different reason—resulting from thermal fluctuations, rather than from quenched disorder.
  • 37
    • 0033246855 scopus 로고    scopus 로고
    • Hence, the possibility of a transition at finite (Formula presented) from many pure states to a single pair, while logically possible, seems unlikely. The presence of such a transition would strongly suggest that the structure of a low-temperature spin glass phase could indeed be different for, say, the Gaussian and (Formula presented) coupling distributions. In this context it is interesting to note that there is a mean-field Hopfield-type model in which the number of pure states is sensitive to the exact distribution of the couplings, but the mechanism there seems to not be relevant to our situation of EA spin glasses; see A. Bovier, B. Niederhauser, and A. van Enter, J. Stat. Phys. 95, 181 (1999).
    • (1999) J. Stat. Phys. , vol.95 , pp. 181
    • Bovier, A.1    Niederhauser, B.2    van Enter, A.3
  • 42
    • 0342746083 scopus 로고
    • There is though a handcrafted example of a lattice field theory with a single ground state but a sequence of temperatures tending to zero with coexisting phases; see E. A. Pecherski and S. B. Shlosman, Theor. Math. Phys. 70, 325 (1987).
    • (1987) Theor. Math. Phys. , vol.70 , pp. 325
    • Pecherski, E.A.1    Shlosman, S.B.2
  • 43
    • 3542995583 scopus 로고
    • However, we emphasize that our claim is not that dimension eight necessarily plays a special role—only that the most likely conclusion of our analysis, of a single pair of low-temperature pure states, holds at least up to eight dimensions
    • The possibility that dimension eight plays a special role in short-ranged spin glasses has been suggested previously, but for different reasons; see D. S. Fisher and H. Sompolinsky, Phys. Rev. Lett. 54, 1063 (1985). However, we emphasize that our claim is not that dimension eight necessarily plays a special role—only that the most likely conclusion of our analysis, of a single pair of low-temperature pure states, holds at least up to eight dimensions.
    • (1985) Phys. Rev. Lett. , vol.54 , pp. 1063
    • Fisher, D.S.1    Sompolinsky, H.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.