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6
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0034339633
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E. Marinari, G. Parisi, F. Ricci-Tersenghi, J. J. Ruiz-Lorenzo, and F. Zuliani, J. Stat. Phys. 98, 973 (2000).
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(2000)
J. Stat. Phys.
, vol.98
, pp. 973
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Marinari, E.1
Parisi, G.2
Ricci-Tersenghi, F.3
Ruiz-Lorenzo, J.J.4
Zuliani, F.5
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19
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85035253709
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A completely rigorous proof, though, has so far been obtained only for (Formula presented)
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A completely rigorous proof, though, has so far been obtained only for (Formula presented).
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21
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85035280067
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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
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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.
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22
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0001632715
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O. Motrunich, S.-C. Mau, D. A. Huse, and D. S. Fisher, Phys. Rev. B 61, 1160 (2000).
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(2000)
Phys. Rev. B
, vol.61
, pp. 1160
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Motrunich, O.1
Mau, S.-C.2
Huse, D.A.3
Fisher, D.S.4
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32
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85035248182
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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
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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.
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37
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0033246855
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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).
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(1999)
J. Stat. Phys.
, vol.95
, pp. 181
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Bovier, A.1
Niederhauser, B.2
van Enter, A.3
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42
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0342746083
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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).
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(1987)
Theor. Math. Phys.
, vol.70
, pp. 325
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Pecherski, E.A.1
Shlosman, S.B.2
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43
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3542995583
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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
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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.
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(1985)
Phys. Rev. Lett.
, vol.54
, pp. 1063
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Fisher, D.S.1
Sompolinsky, H.2
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