-
3
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-
0042974048
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These criteria are of a similar nature as the familiar Harris criterion, which assesses the relevance or irrelevance of random bond bulk disorder; see A.B. Harris, J. Phys. C7, 1671 (1974).
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Harris, A.B.1
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4
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0003130040
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edited by C. Domb, J.L. Lebowitz Academic Press, London
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For background on surface critical behaviour, see H.W. Diehl, in Phase Transitions and Critical Phenomena, edited by C. Domb, J.L. Lebowitz (Academic Press, London, 1986), Vol. 10, pp. 75-267; K. Binder, in Phase Transitions and Critical Phenomena, edited by C. Domb, J.L. Lebowitz (Academic, London, 1983), Vol. 8, pp. 1-144; H.W. Diehl, Int. J. Mod. Phys. B 11, 3593 (1997), preprint cond-mat/9610143.
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(1986)
Phase Transitions and Critical Phenomena
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Diehl, H.W.1
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5
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0001856561
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edited by C. Domb, J.L. Lebowitz Academic, London
-
For background on surface critical behaviour, see H.W. Diehl, in Phase Transitions and Critical Phenomena, edited by C. Domb, J.L. Lebowitz (Academic Press, London, 1986), Vol. 10, pp. 75-267; K. Binder, in Phase Transitions and Critical Phenomena, edited by C. Domb, J.L. Lebowitz (Academic, London, 1983), Vol. 8, pp. 1-144; H.W. Diehl, Int. J. Mod. Phys. B 11, 3593 (1997), preprint cond-mat/9610143.
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(1983)
Phase Transitions and Critical Phenomena
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Binder, K.1
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6
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0009465338
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preprint cond-mat/9610143
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For background on surface critical behaviour, see H.W. Diehl, in Phase Transitions and Critical Phenomena, edited by C. Domb, J.L. Lebowitz (Academic Press, London, 1986), Vol. 10, pp. 75-267; K. Binder, in Phase Transitions and Critical Phenomena, edited by C. Domb, J.L. Lebowitz (Academic, London, 1983), Vol. 8, pp. 1-144; H.W. Diehl, Int. J. Mod. Phys. B 11, 3593 (1997), preprint cond-mat/9610143.
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Int. J. Mod. Phys. B
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Diehl, H.W.1
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0346603727
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C. Ruge, S. Dunkelmann, F. Wagner, J. Wulf, J. Stat. Phys. 73, 293 (1992).
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Ruge, C.1
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Wulf, J.4
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14
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18044388603
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R.B. Griffiths, J. Math. Phys. 8, 478 (1967); D.G. Kelly, S. Sherman, J. Math. Phys. 9, 466 (1968).
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Griffiths, R.B.1
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0002272834
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To my knowledge, not all aspects of these limiting forms have been proven in a mathematically rigorous fashion, but they are consistent with all known results. For rigorous results on the 3D semi-infinite Ising model, see J. Fröhlich, C.-E. Pfister, Commun. Math. Phys. 109, 493 (1987); C.-E. Pfister, O. Penrose, Commun. Math. Phys. 115, 691 (1988).
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Fröhlich, J.1
Pfister, C.-E.2
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17
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0000510370
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-
To my knowledge, not all aspects of these limiting forms have been proven in a mathematically rigorous fashion, but they are consistent with all known results. For rigorous results on the 3D semi-infinite Ising model, see J. Fröhlich, C.-E. Pfister, Commun. Math. Phys. 109, 493 (1987); C.-E. Pfister, O. Penrose, Commun. Math. Phys. 115, 691 (1988).
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Commun. Math. Phys.
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Pfister, C.-E.1
Penrose, O.2
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20
-
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0347744690
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-
note
-
1 becomes unnecessary. It is made here because the assumption of self-averaging is neither required nor used in the derivation of the given inequalities, and not to suggest a possible breakdown of self-averaging.
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22
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0031325696
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W. Selke, F. Szalma, P. Lajkó, F. Iglói, J. Stat. Phys. 89, 1079 (1997); F. Iglói, P. Lajkó, W. Selke, F. Szalma, preprint cond-mat/9711182.
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Selke, W.1
Szalma, F.2
Lajkó, P.3
Iglói, F.4
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23
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0031325696
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preprint cond-mat/9711182
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W. Selke, F. Szalma, P. Lajkó, F. Iglói, J. Stat. Phys. 89, 1079 (1997); F. Iglói, P. Lajkó, W. Selke, F. Szalma, preprint cond-mat/9711182.
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Iglói, F.1
Lajkó, P.2
Selke, W.3
Szalma, F.4
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