2017
DOI: 10.1103/physrevb.96.035142
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Spectrum of the Wilson-Fisher conformal field theory on the torus

Abstract: We study the finite-size spectrum of the O(N ) symmetric Wilson-Fisher conformal field theory (CFT) on the d = 2 spatial-dimension torus using the expansion in = 3 − d. This is done by deriving a set of universal effective Hamiltonians describing fluctuations of the zero momentum modes. The effective Hamiltonians take the form of N -dimensional quantum anharmonic oscillators, which are shown to be strongly coupled at the critical point for small . The low-energy spectrum is solved numerically for N = 1, 2, 3, … Show more

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Cited by 19 publications
(32 citation statements)
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“…The estimated values are about twice the extrapolated values, perhaps indicating non-negligible nonpertubative corrections to ∆ Q for smaller N . However, the conclusion that monopole operators with Q = 1, 2, 3 are relevant (∆ Q < 3) at O(2) fixed point still remains true.FINITE-SIZE SPECTRUMRecently, the universal features in the finite-size critical spectrum of operators have been of interest[31][32][33]. Here, we provide a computation of critical spectrum of Dirac monopole at the O(2) fixed point of XY model.…”
mentioning
confidence: 99%
“…The estimated values are about twice the extrapolated values, perhaps indicating non-negligible nonpertubative corrections to ∆ Q for smaller N . However, the conclusion that monopole operators with Q = 1, 2, 3 are relevant (∆ Q < 3) at O(2) fixed point still remains true.FINITE-SIZE SPECTRUMRecently, the universal features in the finite-size critical spectrum of operators have been of interest[31][32][33]. Here, we provide a computation of critical spectrum of Dirac monopole at the O(2) fixed point of XY model.…”
mentioning
confidence: 99%
“…While the universal description of a critical point is a property of 1D systems (the nature of conformal critical points in 2D is an open question and a subject of cutting-edge numerical studies [10,11]), it has been proposed that critical 1D systems can serve as building blocks of 2D topologically ordered states of matter [12][13][14][15]. Critical 1D systems can be arranged into 2D array and when coupled together in a designed fashion, the system can become a gapped topologically ordered state whose nature depends only on the couplings and on the CFT describing the critical 1D systems.…”
Section: Introductionmentioning
confidence: 99%
“…In fact, another way to identify and chart universality classes is to measure their critical torus energy spectrum as it was shown in Refs. [13][14][15][16] for Wilson-Fisher and topological phase transitions. The low-energy gaps at a relativistic critical point on the torus are given, up to a non-universal factor v describing the effective speed of light, by universal numbers ξ i times 1/L, where L is the linear extent of the cluster [17].…”
Section: Introductionmentioning
confidence: 99%