Boundary conformal field theory at the extraordinary transition: The layer susceptibility to O(ε)

Abstract We present an analytic calculation of the layer (parallel) susceptibility at the extraordinary transition in a semi-infinite system with a flat boundary. Using the method of integral transforms put forward by McAvity and Osborn [Nucl. Phys. B 455 (1995) 522] in the boundary CFT, we derive t...

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Main Author: M. A. Shpot
Format: Article
Language:English
Published: SpringerOpen 2021-01-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP01(2021)055
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spelling doaj-3ad24e638e484d5f99909fd531b4aebd2021-01-17T12:06:53ZengSpringerOpenJournal of High Energy Physics1029-84792021-01-012021112810.1007/JHEP01(2021)055Boundary conformal field theory at the extraordinary transition: The layer susceptibility to O(ε)M. A. Shpot0Institute for Condensed Matter PhysicsAbstract We present an analytic calculation of the layer (parallel) susceptibility at the extraordinary transition in a semi-infinite system with a flat boundary. Using the method of integral transforms put forward by McAvity and Osborn [Nucl. Phys. B 455 (1995) 522] in the boundary CFT, we derive the coordinate-space representation of the mean-field propagator at the transition point. The simple algebraic structure of this function provides a practical possibility of higher-order calculations. Thus we calculate the explicit expression for the layer susceptibility at the extraordinary transition in the one-loop approximation. Our result is correct up to order O(ε) of the ε = 4 − d expansion and holds for arbitrary width of the layer and its position in the half-space. We discuss the general structure of our result and consider the limiting cases related to the boundary operator expansion and (bulk) operator product expansion. We compare our findings with previously known results and less complicated formulas in the case of the ordinary transition. We believe that analytic results for layer susceptibilities could be a good starting point for efficient calculations of two-point correlation functions. This possibility would be of great importance given the recent breakthrough in bulk and boundary conformal field theories in general dimensions.https://doi.org/10.1007/JHEP01(2021)055Boundary Quantum Field TheoryConformal Field TheoryField Theories in Higher DimensionsRenormalization Group
collection DOAJ
language English
format Article
sources DOAJ
author M. A. Shpot
spellingShingle M. A. Shpot
Boundary conformal field theory at the extraordinary transition: The layer susceptibility to O(ε)
Journal of High Energy Physics
Boundary Quantum Field Theory
Conformal Field Theory
Field Theories in Higher Dimensions
Renormalization Group
author_facet M. A. Shpot
author_sort M. A. Shpot
title Boundary conformal field theory at the extraordinary transition: The layer susceptibility to O(ε)
title_short Boundary conformal field theory at the extraordinary transition: The layer susceptibility to O(ε)
title_full Boundary conformal field theory at the extraordinary transition: The layer susceptibility to O(ε)
title_fullStr Boundary conformal field theory at the extraordinary transition: The layer susceptibility to O(ε)
title_full_unstemmed Boundary conformal field theory at the extraordinary transition: The layer susceptibility to O(ε)
title_sort boundary conformal field theory at the extraordinary transition: the layer susceptibility to o(ε)
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2021-01-01
description Abstract We present an analytic calculation of the layer (parallel) susceptibility at the extraordinary transition in a semi-infinite system with a flat boundary. Using the method of integral transforms put forward by McAvity and Osborn [Nucl. Phys. B 455 (1995) 522] in the boundary CFT, we derive the coordinate-space representation of the mean-field propagator at the transition point. The simple algebraic structure of this function provides a practical possibility of higher-order calculations. Thus we calculate the explicit expression for the layer susceptibility at the extraordinary transition in the one-loop approximation. Our result is correct up to order O(ε) of the ε = 4 − d expansion and holds for arbitrary width of the layer and its position in the half-space. We discuss the general structure of our result and consider the limiting cases related to the boundary operator expansion and (bulk) operator product expansion. We compare our findings with previously known results and less complicated formulas in the case of the ordinary transition. We believe that analytic results for layer susceptibilities could be a good starting point for efficient calculations of two-point correlation functions. This possibility would be of great importance given the recent breakthrough in bulk and boundary conformal field theories in general dimensions.
topic Boundary Quantum Field Theory
Conformal Field Theory
Field Theories in Higher Dimensions
Renormalization Group
url https://doi.org/10.1007/JHEP01(2021)055
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