Finite-Temperature Conformal Field Theory Results for All Couplings: O(N) Model in 2+1 Dimensions
Apr 22, 20195 pages
Published in:
- Phys.Rev.Lett. 122 (2019) 23, 231603,
- Phys.Rev.Lett. 123 (2019) 20, 209901 (erratum)
- Published: Jun 14, 2019
e-Print:
- 1904.09995 [hep-th]
DOI:
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Abstract: (APS)
A famous example of gauge-gravity duality is the result that the entropy density of the strongly coupled N=4 supersymmetric Yang-Mills theory in four dimensions for large N is exactly 3/4 of the Stefan-Boltzmann limit. In this work, I revisit the massless O(N) model in 2+1 dimensions, which is analytically solvable at a finite-temperature T for all couplings λ in the large N limit. I find that the entropy density monotonically decreases from the Stefan-Boltzmann limit at λ=0 to exactly 4/5 of the Stefan-Boltzmann limit at λ=∞. Calculating the retarded energy-momentum tensor correlator in the scalar channel at λ=∞, I find that it has two logarithmic branch cuts originating at ω=±4Tln(1+5/2) but no singularities in the whole complex frequency plane. I show that the ratio 4/5 and the location of the branch points both are universal within a large class of bosonic conformal field theories in 2+1 dimensions.Note:
- 5 pages, 1 figure; v2: typos fixed, new section on universality of 4/5 ratio; v3: matches published version; v4: typos/errors corrected
- Elementary Particles and Fields
- dimension: 4
- gravitation: duality
- entropy: density
- dimension: 3
- model: O(N)
- field theory: conformal
- finite temperature
- strong coupling
- expansion 1/N
References(16)
Figures(1)
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