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1
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58149319544
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D. Kivelson, S. A. Kivelson, X. L. Zhao, Z. Nussinov, and G. Tarjus, Physica A 219, 27 (1995);
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Physica A
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Kivelson, D.1
Kivelson, S.A.2
Zhao, X.L.3
Nussinov, Z.4
Tarjus, G.5
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15
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0001223227
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U. Low, V. J. Emery, K. Fabricius, and S. A. Kivelson, Phys. Rev. Lett. 72, 1918 (1994).
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Phys. Rev. Lett.
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Low, U.1
Emery, V.J.2
Fabricius, K.3
Kivelson, S.A.4
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22
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85036281894
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One should note that (Formula presented) is very close to (Formula presented) the relative difference being less than (Formula presented) in the small frustration range, (Formula presented)
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One should note that (Formula presented) is very close to (Formula presented) the relative difference being less than (Formula presented) in the small frustration range, (Formula presented).
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23
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85036313606
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W. Götze, in Liquids, Freezing and the Glass Transition, edited by J. P. H. D. Levesque and J. Zinn-Justin (North Holland, Amsterdam, 1991), p. 287
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W. Götze, in Liquids, Freezing and the Glass Transition, edited by J. P. H. D. Levesque and J. Zinn-Justin (North Holland, Amsterdam, 1991), p. 287.
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26
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30244435648
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J. P. Bouchaud, L. Cugliandolo, J. Kurchan, and M. Mézard, Physica A 226, 243 (1996).
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Physica A
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Bouchaud, J.P.1
Cugliandolo, L.2
Kurchan, J.3
Mézard, M.4
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30
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85036355813
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For a field theory with n-component fields with (Formula presented) symmetry, the Hartree approximation takes into account all diagrams that survive in the (Formula presented) limit whereas the SCSA includes in a self-consistent manner the leading (Formula presented) corrections. In the present case, one is of course interested by (Formula presented)
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For a field theory with n-component fields with (Formula presented) symmetry, the Hartree approximation takes into account all diagrams that survive in the (Formula presented) limit whereas the SCSA includes in a self-consistent manner the leading (Formula presented) corrections. In the present case, one is of course interested by (Formula presented).
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31
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85036383970
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Contrary to those two approximations that retain some of the non-linearities of the dynamics, the dynamical counterpart of the Hartree approximation leads to an essentially linear equation, and it is not further considered in this work
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Contrary to those two approximations that retain some of the non-linearities of the dynamics, the dynamical counterpart of the Hartree approximation leads to an essentially linear equation, and it is not further considered in this work.
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33
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0011932195
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M. Fuchs, W. Götze, I. Hofacker, and A. Latz, J. Phys.: Condens. Matter 3, 5047 (1991).
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(1991)
J. Phys.: Condens. Matter
, vol.3
, pp. 5047
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Fuchs, M.1
Götze, W.2
Hofacker, I.3
Latz, A.4
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34
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85036266892
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V. Krakoviack, Ph.D. thesis, University of Paris Sud, Orsay, France (2000)
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V. Krakoviack, Ph.D. thesis, University of Paris Sud, Orsay, France (2000).
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36
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85036379486
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Note that the same considerations apply to the replica approach of the glassy state of simple liquids, where nontrivial behavior can be found with the hypernetted chain approximation, but not with the “too linear” Percus-Yevick and mean-spherical approximations 12
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Note that the same considerations apply to the replica approach of the glassy state of simple liquids, where nontrivial behavior can be found with the hypernetted chain approximation, but not with the “too linear” Percus-Yevick and mean-spherical approximations 12.
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