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see also Ref. 1
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K. Binder and P. C. Hohenberg, Phys. Rev. B6, 3461 (1972); H. Au-Yang and M. E. Fisher, Phys. Rev. B11, 3469 (1975); see also Ref. 1.
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5844252202
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H. Au-Yang, J. Math. Phys. 14, 937 (1973); H. Au-Yang and M. E. Fisher. Phys. Rev. B21, 3956 (1980).
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Au-Yang, H.1
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Chatterjee, R.1
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19
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85033132672
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note
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In Ref. 5 the surface exponents were additionally labelled with the superscript "ord" in order to distinguish exponents of the various surface universality classes existing in d = 3. Since in the present work we focus on d = 2, this distinction is not necessary; the surface exponents appearing all belong to the universality class of the ordinary transition.
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20
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0002299935
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K. Symanzyk, Nucl. Phys. B190 [FS3], 1 (1981); H. W. Diehl and S. Dietrich, Z. Phys. B42, 65 (1981).
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Cardy, J.L.1
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0003476862
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North-Holland, Amsterdam, for an overview
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See e.g. J. F. Cardy, Finite Size Scaling (North-Holland, Amsterdam, 1988) for an overview.
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Wang, J.-S.1
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85033148161
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note
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1 have different values.
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29
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0000443253
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X. Mailänder, H. Dosch, J. Peisl and R. L. Johnson, Phys. Rev. Lett. 64, 2527 (1990).
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31
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85033127294
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note
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13 examined a slightly more general system with different coupling strengths in directions parallel and perpendicular to the surface. We restrict our presentation to the isotropic case.
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