2009
DOI: 10.1090/pcms/016/02
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Lectures on the renormalisation group

Abstract: Lecture 4. Renormalisation group for Euclidean models 4.1. Euclidean Lattice and the Dipole Model 4.2. The Initial I 0 , K 0 4.3. The Basic Scaling Mechanism 4.4. Coordinates (I j , K j) 4.5. Euclidean Replacement for Lemma 2.14 i ii LECTURE 0. CONTENTS Lecture 5. Coordinates and action of renormalisation group 5.1. Euclidean Replacement for Lemma 2.14 continued 5.2. Formulas forĨ, J.

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Cited by 49 publications
(128 citation statements)
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“…where m > 0 and ∇ is the discrete gradient operator acting on fields φ : Z d → R. In the case when V (z) = |z| 2 /2 + a d j=1 cos z j , z ∈ R d , the probability measure (1.2) describes the dual representation of a gas of lattice dipoles with activity a (see [3]). Our estimates on fluctuations will be uniform for m > 0.…”
Section: Introductionmentioning
confidence: 99%
“…where m > 0 and ∇ is the discrete gradient operator acting on fields φ : Z d → R. In the case when V (z) = |z| 2 /2 + a d j=1 cos z j , z ∈ R d , the probability measure (1.2) describes the dual representation of a gas of lattice dipoles with activity a (see [3]). Our estimates on fluctuations will be uniform for m > 0.…”
Section: Introductionmentioning
confidence: 99%
“…We now claim that from (53) we obtain (55): If we smuggle in (55) the weight |x − y| α 2 q and apply Hölder's inequality first in x and then in y, we get 6 To show Sobolev's inequality in the outer domain {|x| > R} we argue as follows: By scale invariance, we may reduce ourselves to the domain {|x| > 1}; moreover, by standard approximation, we may assume u to be smooth and zero outside a ball big enough. We now extend u inside {|x| < 1} using the radial reflection x → x |x| 2 , apply Sobolev's inequality on the whole space and conclude by observing that, due to our choice of extension, the Dirichlet integral in {|x| < 1} can be controlled by the Dirichlet integral in {|x| > 1}.…”
Section: Proof Of Theoremmentioning
confidence: 94%
“…A different approach that is related to the scale-invariance of Z d is the renormalization group method, which has been very useful for several statistical physics models at criticality; see [Bry07]. We will not discuss this approach here.…”
Section: Percolation Renormalization and Scale-invariant Tilingsmentioning
confidence: 99%