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5
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Mézard, M.1
Zecchina, R.2
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11
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0346604644
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note
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(1). Solving the previous equation we recover Eq. (7). Under this last form the argument may be easily generalized to lattices with random connectivity.
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17
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0002171519
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J. T. Chayes, L. Chayes, J. P. Sethna, and D. J. Thouless, Commun. Math. Phys. 106:41 (1986); J. M. Carlson, J. T. Chayes, L. Chayes, J. P. Sethna, and D. J. Thouless, Europhys. Lett. 5:355 (1988).
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Chayes, J.T.1
Chayes, L.2
Sethna, J.P.3
Thouless, D.J.4
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18
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84956110307
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J. T. Chayes, L. Chayes, J. P. Sethna, and D. J. Thouless, Commun. Math. Phys. 106:41 (1986); J. M. Carlson, J. T. Chayes, L. Chayes, J. P. Sethna, and D. J. Thouless, Europhys. Lett. 5:355 (1988).
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Carlson, J.M.1
Chayes, J.T.2
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Thouless, D.J.5
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21
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22244449280
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J. M. Carlson, J. T. Chayes, L. Chayes, J. P. Sethna, and D. J. Thouless, J. Statist. Phys. 61:987 (1990); J. M. Carlson, J. T. Chayes, J. P. Sethna, and D. J. Thouless, J. Statist. Phys. 61:1069 (1990).
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Carlson, J.M.1
Chayes, J.T.2
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Thouless, D.J.5
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22
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0011550362
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J. M. Carlson, J. T. Chayes, L. Chayes, J. P. Sethna, and D. J. Thouless, J. Statist. Phys. 61:987 (1990); J. M. Carlson, J. T. Chayes, J. P. Sethna, and D. J. Thouless, J. Statist. Phys. 61:1069 (1990).
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Thouless, D.J.4
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23
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0345973298
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note
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It is easy to check that this expression is equal to the zero temperature limit of the general finite temperature iteration formula used in ref. 9.
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29
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4243446634
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C. De Dominicis and Y. Y. Goldschmidt, J. Phys. A 22:L775 (1989) and Phys. Rev. B 41:2184 (1990).
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32
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0347864719
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note
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One could use the expression imprecise probabilities to describe this situation.
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40
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39249085744
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43
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0019061437
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Orland, H.4
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