A Three-Dimensional Conformal Field Theory

dc.creatorGuruswamy, S.
dc.creatorRajeev, S. G.
dc.creatorVitale, P.
dc.date1994-08-04
dc.date.accessioned2026-07-07T03:07:23Z
dc.date.available2026-07-07T03:07:23Z
dc.descriptionThis talk is based on a recent paper$^{1}$ of ours. In an attempt to understand three-dimensional conformal field theories, we study in detail one such example --the large $N$ limit of the $O(N)$ non-linear sigma model at its non-trivial fixed point -- in the zeta function regularization. We study this on various three-dimensional manifolds of constant curvature of the kind $Σ\times R$ ($Σ=S^1 \times S^1, S^2, H^2$). This describes a quantum phase transition at zero temperature. We illustrate that the factor that determines whether $m=0$ or not at the critical point in the different cases is not the `size' of $Σ$ or its Riemannian curvature, but the conformal class of the metric.
dc.description7 pages, TeX, UR-1368/ER-40685-818 (Talk presented by S.G. at the 16-th Annual Montreal-Rochester-Syracuse- Toronto (MRST) Meeting:``What Next? Exploring the Future of High-Energy Physics'', held at McGill University, Montreal, Canada, 11--13 May 1994. To appear in Proceedings published by World Scientific.)
dc.identifierhttps://arxiv.org/abs/cond-mat/9408018
dc.identifierhttp://arxiv.org/abs/cond-mat/9408018
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/27152
dc.subjectCondensed Matter
dc.subjectHigh Energy Physics - Theory
dc.titleA Three-Dimensional Conformal Field Theory
dc.typetext

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