AIP Conference Proceedings 1973
DOI: 10.1063/1.2947035
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Critical Phenomena in 3.99 Dimensions

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1976
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Cited by 4 publications
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“…K. G. Wilson gave the talk ‘Critical Phenomena in 3.99 Dimensions’ where he explained in more detail how renormalization theory could overcome the breakdown of Landau theory. Apart from inducing a flood of calculations of critical exponents in various systems, Wilson’s theory not only “gave new life to the theory of critical phenomena” [ 45 ] but led also advance in other fields like high-energy physics or physics of turbulence. This wide-reaching aspect is reflected in the citation rate (see Figure 4 a) and recently in Paul Fendley’s judgment: “The RG is not only the way to understand critical phenomena quantitatively, but lies at the very core of why theoretical physics is so effective” [ 46 ].…”
Section: Sharing Science In the Time Of The Cold Warmentioning
confidence: 99%
“…K. G. Wilson gave the talk ‘Critical Phenomena in 3.99 Dimensions’ where he explained in more detail how renormalization theory could overcome the breakdown of Landau theory. Apart from inducing a flood of calculations of critical exponents in various systems, Wilson’s theory not only “gave new life to the theory of critical phenomena” [ 45 ] but led also advance in other fields like high-energy physics or physics of turbulence. This wide-reaching aspect is reflected in the citation rate (see Figure 4 a) and recently in Paul Fendley’s judgment: “The RG is not only the way to understand critical phenomena quantitatively, but lies at the very core of why theoretical physics is so effective” [ 46 ].…”
Section: Sharing Science In the Time Of The Cold Warmentioning
confidence: 99%
“…However, situations where we introduce some degree of dilution (e.g. Erdös-Rényi graph), yet preserving the homogeneity of the structure and an extensive coordination number, can be looked and treated as mean field models.2 In that context the long-range interactions are unacceptable because the involved couplings are of electromagnetic nature, hence displaying power-law decay with the distance.3 It is worth mentioning that the Wilson-Kadanoff renormalization equations [37,38,39] turn out to be exact in models with power law interactions as those built on the hierarchical lattice that we are going to consider. 2 k+1 i<j brings a contribution scaling like 2 2(k+1) ∼ N 2 , while the pre-factor scales as 2 −2σ(k+1) ∼ N −2σ , thus, when σ < 1 2 the intensive energy is overall divergent in the thermodynamic limit k → ∞.…”
mentioning
confidence: 99%
“…3 It is worth mentioning that the Wilson-Kadanoff renormalization equations [37,38,39] turn out to be exact in models with power law interactions as those built on the hierarchical lattice that we are going to consider. 2 k+1 i<j brings a contribution scaling like 2 2(k+1) ∼ N 2 , while the pre-factor scales as 2 −2σ(k+1) ∼ N −2σ , thus, when σ < 1 2 the intensive energy is overall divergent in the thermodynamic limit k → ∞.…”
mentioning
confidence: 99%