
In renormalized field theories there are in general one or few fixed points which are accessible by the renormalization-group flow. They can be identified from the fixed-point equations. Exceptionally, an infinite family of fixed points exists, parameterized by a scaling exponent $��$, itself function of a non-renormalizing parameter. Here we report a different scenario with an infinite family of fixed points of which seemingly only one is chosen by the renormalization-group flow. This dynamical selection takes place in systems with an attractive interaction ${\cal V}(��)$, as in standard $��^4$ theory, but where the potential $\cal V$ at large $��$ goes to zero, as e.g. the attraction by a defect.
v2: Several misprints corrected, appendix on toy model rendered more relevant. 13 pages, 22 figures
High Energy Physics - Theory, Statistical Mechanics (cond-mat.stat-mech), High Energy Physics - Theory (hep-th), FOS: Physical sciences, Condensed Matter - Statistical Mechanics, [PHYS] Physics [physics]
High Energy Physics - Theory, Statistical Mechanics (cond-mat.stat-mech), High Energy Physics - Theory (hep-th), FOS: Physical sciences, Condensed Matter - Statistical Mechanics, [PHYS] Physics [physics]
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