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The Fixed Point of a Generalization of the Renormalization Group Maps for Self-Avoiding Paths on Gaskets
Authors:Tetsuya Hattori
Affiliation:(1) Mathematical Institute, Graduate School of Science, Tohoku University, Aoba-ku, Sendai 980–8578, Japan
Abstract:
Let W(x,y) = ax 3+ bx 4+ f 5 x 5+ f 6 x 6+ (3 ax 2)2 y+ g 5 x 5 y + h 3 x 3 y 2 + h 4 x 4 y 2 + n 3 x 3 y 3+a 24 x 2 y 4+a 05 y 5+a 15 xy 5+a 06 y 6, and X = $$ X={frac{partial{W}}{partial{x}}}$$, $$ Y={frac{partial{W}}{partial{y}}}$$, where the coefficients are non-negative constants, with a > 0, such that X 2(x,x 2)−Y(x,x 2) is a polynomial of x with non-negative coefficients. Examples of the 2 dimensional map Φ: (x,y)↦ (X(x,y),Y(x,y)) satisfying the conditions are the renormalization group (RG) maps (modulo change of variables) for the restricted self-avoiding paths on the 3 and 4 dimensional pre-gaskets. We prove that there exists a unique fixed point (x f ,y f ) of Φ in the invariant set $${(x,y)in{mathbb R}^2mid x^2 geqq y} setminusbackslash {0}$$. 2000 Mathematics Subject Classification Numbers: 82B28; 60G99; 81T17; 82C41.
Keywords:renormalization group  fixed point uniqueness  self-avoiding paths  Sierpinski gasket
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