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Exact scheme independence at two loops

We further develop an algorithmic and diagrammatic computational framework for very general exact renormalization groups, where the embedded regularisation scheme, parametrised by a general cutoff function and infinitely many higher point vertices, is left unspecified. Calculations proceed iterative...

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Detalles Bibliográficos
Autores principales: Arnone, S, Gatti, A, Morris, T R, Rosten, O J
Lenguaje:eng
Publicado: 2003
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.69.065009
http://cds.cern.ch/record/645327
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author Arnone, S
Gatti, A
Morris, T R
Rosten, O J
author_facet Arnone, S
Gatti, A
Morris, T R
Rosten, O J
author_sort Arnone, S
collection CERN
description We further develop an algorithmic and diagrammatic computational framework for very general exact renormalization groups, where the embedded regularisation scheme, parametrised by a general cutoff function and infinitely many higher point vertices, is left unspecified. Calculations proceed iteratively, by integrating by parts with respect to the effective cutoff, thus introducing effective propagators, and differentials of vertices that can be expanded using the flow equations; many cancellations occur on using the fact that the effective propagator is the inverse of the classical Wilsonian two-point vertex. We demonstrate the power of these methods by computing the beta function up to two loops in massless four dimensional scalar field theory, obtaining the expected universal coefficients, independent of the details of the regularisation scheme.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2003
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spelling cern-6453272019-09-30T06:29:59Zdoi:10.1103/PhysRevD.69.065009http://cds.cern.ch/record/645327engArnone, SGatti, AMorris, T RRosten, O JExact scheme independence at two loopsParticle Physics - TheoryWe further develop an algorithmic and diagrammatic computational framework for very general exact renormalization groups, where the embedded regularisation scheme, parametrised by a general cutoff function and infinitely many higher point vertices, is left unspecified. Calculations proceed iteratively, by integrating by parts with respect to the effective cutoff, thus introducing effective propagators, and differentials of vertices that can be expanded using the flow equations; many cancellations occur on using the fact that the effective propagator is the inverse of the classical Wilsonian two-point vertex. We demonstrate the power of these methods by computing the beta function up to two loops in massless four dimensional scalar field theory, obtaining the expected universal coefficients, independent of the details of the regularisation scheme.hep-th/0309242CERN-TH-2003-264SHEP-2003-17oai:cds.cern.ch:6453272003-09-26
spellingShingle Particle Physics - Theory
Arnone, S
Gatti, A
Morris, T R
Rosten, O J
Exact scheme independence at two loops
title Exact scheme independence at two loops
title_full Exact scheme independence at two loops
title_fullStr Exact scheme independence at two loops
title_full_unstemmed Exact scheme independence at two loops
title_short Exact scheme independence at two loops
title_sort exact scheme independence at two loops
topic Particle Physics - Theory
url https://dx.doi.org/10.1103/PhysRevD.69.065009
http://cds.cern.ch/record/645327
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AT morristr exactschemeindependenceattwoloops
AT rostenoj exactschemeindependenceattwoloops