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Anomalies, Unitarity and Quantum Irreversibility

The trace anomaly in external gravity is the sum of three terms at criticality: the square of the Weyl tensor, the Euler density and Box R, with coefficients, properly normalized, called c, a and a', the latter being ambiguously defined by an additive constant. Unitarity and positivity properti...

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Autor principal: Anselmi, Damiano
Lenguaje:eng
Publicado: 1999
Materias:
Acceso en línea:https://dx.doi.org/10.1006/aphy.1999.5949
http://cds.cern.ch/record/381045
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author Anselmi, Damiano
author_facet Anselmi, Damiano
author_sort Anselmi, Damiano
collection CERN
description The trace anomaly in external gravity is the sum of three terms at criticality: the square of the Weyl tensor, the Euler density and Box R, with coefficients, properly normalized, called c, a and a', the latter being ambiguously defined by an additive constant. Unitarity and positivity properties of the induced actions allow us to show that the total RG flows of a and a' are equal and therefore the a'-ambiguity can be consistently removed through the identification a'=a. The picture that emerges clarifies several long-standing issues. The interplay between unitarity and renormalization implies that the flux of the renormalization group is irreversible. A monotonically decreasing a-function interpolating between the appropriate values is naturally provided by a'. The total a-flow is expressed non-perturbatively as the invariant (i.e. scheme-independent) area of the graph of the beta function between the fixed points. We test this prediction to the fourth loop order in perturbation theory, in QCD with Nf ~< 11/2 Nc and in supersymmetric QCD. There is agreement also in the absence of an interacting fixed point (QED and phi^4-theory). Our arguments do not seem to prove that a is strictly positive, but put a lower bound to its value.
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spelling cern-3810452021-10-08T02:31:12Zdoi:10.1006/aphy.1999.5949http://cds.cern.ch/record/381045engAnselmi, DamianoAnomalies, Unitarity and Quantum IrreversibilityParticle Physics - TheoryThe trace anomaly in external gravity is the sum of three terms at criticality: the square of the Weyl tensor, the Euler density and Box R, with coefficients, properly normalized, called c, a and a', the latter being ambiguously defined by an additive constant. Unitarity and positivity properties of the induced actions allow us to show that the total RG flows of a and a' are equal and therefore the a'-ambiguity can be consistently removed through the identification a'=a. The picture that emerges clarifies several long-standing issues. The interplay between unitarity and renormalization implies that the flux of the renormalization group is irreversible. A monotonically decreasing a-function interpolating between the appropriate values is naturally provided by a'. The total a-flow is expressed non-perturbatively as the invariant (i.e. scheme-independent) area of the graph of the beta function between the fixed points. We test this prediction to the fourth loop order in perturbation theory, in QCD with Nf ~< 11/2 Nc and in supersymmetric QCD. There is agreement also in the absence of an interacting fixed point (QED and phi^4-theory). Our arguments do not seem to prove that a is strictly positive, but put a lower bound to its value.The trace anomaly in external gravity is the sum of three terms at criticality: the square of the Weyl tensor, the Euler density and Box R, with coefficients, properly normalized, called c, a and a', the latter being ambiguously defined by an additive constant. Considerations about unitarity and positivity properties of the induced actions allow us to show that the total RG flows of a and a' are equal and therefore the a'-ambiguity can be consistently removed through the identification a'=a. The picture that emerges clarifies several long-standing issues. The interplay between unitarity and renormalization implies that the flux of the renormalization group is irreversible. A monotonically decreasing a-function interpolating between the appropriate values is naturally provided by a'. The total a-flow is expressed non-perturbatively as the invariant (i.e. scheme-independent) area of the graph of the beta function between the fixed points. We test this prediction to the fourth loop order in perturbation theory, in QCD with Nf ~< 11/2 Nc and in supersymmetric QCD. There is agreement also in the absence of an interacting fixed point (QED and phi^4-theory). Arguments for the positivity of a are also discussed.The trace anomaly in external gravity is the sum of three terms at criticality: the square of the Weyl tensor, the Euler density and Box R, with coefficients, properly normalized, called c, a and a', the latter being ambiguously defined by an additive constant. Considerations about unitarity and positivity properties of the induced actions allow us to show that the total RG flows of a and a' are equal and therefore the a'-ambiguity can be consistently removed through the identification a'=a. The picture that emerges clarifies several long-standing issues. The interplay between unitarity and renormalization implies that the flux of the renormalization group is irreversible. A monotonically decreasing a-function interpolating between the appropriate values is naturally provided by a'. The total a-flow is expressed non-perturbatively as the invariant (i.e. scheme-independent) area of the graph of the beta function between the fixed points. We test this prediction to the fourth loop order in perturbation theory, in QCD with Nf ~< 11/2 Nc and in supersymmetric QCD. There is agreement also in the absence of an interacting fixed point (QED and phi^4-theory). Arguments for the positivity of a are also discussed.The trace anomaly in external gravity is the sum of three terms at criticality: the square of the Weyl tensor, the Euler density and □ R , with coefficients, properly normalized, called c , a , and a ′, the latter being ambiguously defined by an additive constant. Considerations about unitarity and positivity properties of the induced actions allow us to show that the total RG flows of a and a ′ are equal and therefore the a ′-ambiguity can be consistently removed through the identification a ′= a . The picture that emerges clarifies several long-standing issues. The interplay between unitarity and renormalization implies that the flux of the renormalization group is irreversible. A monotonically decreasing a -function interpolating between the appropriate values is naturally provided by a ′. The total a -flow is expressed non-perturbatively as the invariant (i.e., scheme-independent) area of the graph of the beta function between the fixed points. We test this prediction to the fourth loop order in perturbation theory, in QCD with N f ≲11/2 N c and in supersymmetric QCD. There is agreement also in the absence of an interacting fixed point (QED and ϕ 4 -theory). Arguments for the positivity of a are also discussed.hep-th/9903059CERN-TH-99-33CERN-TH-99-033oai:cds.cern.ch:3810451999-03-09
spellingShingle Particle Physics - Theory
Anselmi, Damiano
Anomalies, Unitarity and Quantum Irreversibility
title Anomalies, Unitarity and Quantum Irreversibility
title_full Anomalies, Unitarity and Quantum Irreversibility
title_fullStr Anomalies, Unitarity and Quantum Irreversibility
title_full_unstemmed Anomalies, Unitarity and Quantum Irreversibility
title_short Anomalies, Unitarity and Quantum Irreversibility
title_sort anomalies, unitarity and quantum irreversibility
topic Particle Physics - Theory
url https://dx.doi.org/10.1006/aphy.1999.5949
http://cds.cern.ch/record/381045
work_keys_str_mv AT anselmidamiano anomaliesunitarityandquantumirreversibility