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Classical and quantum behavior in mean-field glassy systems
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35
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0346517510
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note
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mcp) = (0.37506, 0.95379)J.
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37
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0000910155
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C. Domb, J.L. Lebowitz (Eds.), Academic, New York
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G. Forgacs, R. Lipowsky, Th.M. Nieuwenhuizen, in: C. Domb, J.L. Lebowitz (Eds.), Phase Transitions and Critical Phenomena vol. 14, Academic, New York, 1991, pp. 135.
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Forgacs, G.1
Lipowsky, R.2
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48
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0347777975
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note
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Regularisation terms correspond to M dependent expressions which yield the same M → ∞ limit.
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57
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0345886703
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preprint cond-mat/9705297
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For a recent investigation see also, P. Sen, P. Ray, B.K. Chakrabarti, preprint cond-mat/9705297.
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Sen, P.1
Ray, P.2
Chakrabarti, B.K.3
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61
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0345886702
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note
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d(t - t′) to be time independent.
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62
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0345886704
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note
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We suppose that the size of the system is infinite from the begining or that the typical time scale involved in the adiabatic process grows with the size of the system much slower than any exponentially long time scale. Obviously, for weak first order phase transitions this assertion is no longer true.
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