2020
DOI: 10.48550/arxiv.2010.07096
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The Coleman correspondence at the free fermion point

Abstract: We prove that the truncated correlation functions of the charge and gradient fields associated with the massless sine-Gordon model on R 2 with β = 4π exist for all coupling constants and are equal to those of the chiral densities and vector current of free massive Dirac fermions. This is an instance of Coleman's prediction that the massless sine-Gordon model and the massive Thirring model are equivalent (in the above sense of correlation functions). Our main novelty is that we prove this correspondence in the … Show more

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Cited by 4 publications
(5 citation statements)
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“…Indeed, the two-point function of the gradient of the discrete GFF is known to decay like the inverse square of the distance (see e.g. [6]).…”
Section: 5mentioning
confidence: 99%
“…Indeed, the two-point function of the gradient of the discrete GFF is known to decay like the inverse square of the distance (see e.g. [6]).…”
Section: 5mentioning
confidence: 99%
“…(E.g., see [4, Section 2.7] for a relevant discussion under the additional assumption ϑ ∈ R specific to the Ising model setup.) In the theoretical physics language, in this setup the limit of height fluctuations should be described by the bosonization of free massive fermions, which leads to the sine-Gordon theory with a special value of the interaction parameter rather than to free bosons; e.g., see [1] and references therein. Coming back to the dimer model language, this means that we do not expect the height fluctuations to have a Gaussian structure in the small mesh size limit if m(ζ) = 0; cf.…”
Section: [±±]mentioning
confidence: 99%
“…Remarkably, many of the models listed here have non-Gaussian or non-determinantal infrared fixed points, and results are robust under a large class of microscopic perturbations of the lattice Hamiltonian. Moreover, this approach led to the proof of several predictions from CFT, such as scaling relations among critical exponents and amplitudes [10,28], bosonization identities [5,7], and expression for the universal subleading contributions to the critical free energy [24]. A limitation of this approach is that it is restricted to 'weakly interacting' cases, that is, to models that are close to a Gaussian model or to a free Fermi model.…”
Section: Introductionmentioning
confidence: 99%