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Nonperturbative running of the quark mass for $N$$_{f}$ = 3 QCD from the chirally rotated Schrödinger functional

We study the renormalization group (RG) running of the quark mass, for <math display="inline"><msub><mi>N</mi><mi>f</mi></msub><mo>=</mo><mn>3</mn></math> QCD with Wilson fermions in a mixed action setup, with standard...

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Autores principales: Plasencia, Isabel Campos, Brida, Mattia Dalla, de Divitiis, Giulia Maria, Lytle, Andrew, Papinutto, Mauro, Pirelli, Ludovica, Vladikas, Anastassios
Lenguaje:eng
Publicado: 2021
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.105.054506
http://cds.cern.ch/record/2798578
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author Plasencia, Isabel Campos
Brida, Mattia Dalla
de Divitiis, Giulia Maria
Lytle, Andrew
Papinutto, Mauro
Pirelli, Ludovica
Vladikas, Anastassios
author_facet Plasencia, Isabel Campos
Brida, Mattia Dalla
de Divitiis, Giulia Maria
Lytle, Andrew
Papinutto, Mauro
Pirelli, Ludovica
Vladikas, Anastassios
author_sort Plasencia, Isabel Campos
collection CERN
description We study the renormalization group (RG) running of the quark mass, for <math display="inline"><msub><mi>N</mi><mi>f</mi></msub><mo>=</mo><mn>3</mn></math> QCD with Wilson fermions in a mixed action setup, with standard Schrödinger functional (SF) boundary conditions for sea quarks and chirally rotated Schrödinger functional (<math display="inline"><mrow><mi>χ</mi><mi>SF</mi></mrow></math>) boundary conditions for valence quarks. This necessitates the tuning of the boundary factor <math display="inline"><msub><mi>z</mi><mi mathvariant="normal">f</mi></msub><mo stretchy="false">(</mo><msubsup><mi>g</mi><mn>0</mn><mn>2</mn></msubsup><mo stretchy="false">)</mo></math> of the <math display="inline"><mrow><mi>χ</mi><mi>SF</mi></mrow></math> valence action, in order to ensure that QCD symmetries are fully recovered in the continuum. The properties of this novel setup are monitored through the ratios <math display="inline"><msub><mi>Z</mi><mi>S</mi></msub><mo>/</mo><msub><mi>Z</mi><mi>P</mi></msub></math> and <math display="inline"><msub><mi mathvariant="normal">Σ</mi><mi>S</mi></msub><mo>/</mo><msub><mi mathvariant="normal">Σ</mi><mi>P</mi></msub></math> of the renormalization parameters and step scaling functions of the scalar and pseudoscalar densities. Where comparison is possible, our <math display="inline"><msub><mi>Z</mi><mi>S</mi></msub><mo>/</mo><msub><mi>Z</mi><mi>P</mi></msub></math> results are found to agree with previous determinations, based on a mass ratio method [G. M. de Divitiis (ALPHA Collaboration), Eur. Phys. J. C 79, 797 (2019)] and Ward identities [ J. Heitger (ALPHA Collaboration), Eur. Phys. J. C 80, 765 (2020); J. Heitger , Eur. Phys. J. C 81, 606 (2021)], with Schrödinger functional boundary conditions. The behavior of <math display="inline"><msub><mi mathvariant="normal">Σ</mi><mi>S</mi></msub><mo>/</mo><msub><mi mathvariant="normal">Σ</mi><mi>P</mi></msub></math> confirms the theoretical expectations of <math display="inline"><mrow><mi>χ</mi><mi>SF</mi></mrow></math> QCD, related to the restoration of the theory’s symmetries in the continuum limit. From the step-scaling function of the pseudoscalar density we obtain the quark mass RG-running function from hadronic to perturbative energy scales. This is fully compatible with the earlier result obtained in a similar setup for Wilson quarks with Schrödinger functional boundary conditions [I. Campos , Eur. Phys. J. C 78, 387 (2018)], and provides a strong universality test for the two lattice setups.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2021
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spelling cern-27985782023-08-11T04:12:52Zdoi:10.1103/PhysRevD.105.054506http://cds.cern.ch/record/2798578engPlasencia, Isabel CamposBrida, Mattia Dallade Divitiis, Giulia MariaLytle, AndrewPapinutto, MauroPirelli, LudovicaVladikas, AnastassiosNonperturbative running of the quark mass for $N$$_{f}$ = 3 QCD from the chirally rotated Schrödinger functionalhep-latParticle Physics - LatticeWe study the renormalization group (RG) running of the quark mass, for <math display="inline"><msub><mi>N</mi><mi>f</mi></msub><mo>=</mo><mn>3</mn></math> QCD with Wilson fermions in a mixed action setup, with standard Schrödinger functional (SF) boundary conditions for sea quarks and chirally rotated Schrödinger functional (<math display="inline"><mrow><mi>χ</mi><mi>SF</mi></mrow></math>) boundary conditions for valence quarks. This necessitates the tuning of the boundary factor <math display="inline"><msub><mi>z</mi><mi mathvariant="normal">f</mi></msub><mo stretchy="false">(</mo><msubsup><mi>g</mi><mn>0</mn><mn>2</mn></msubsup><mo stretchy="false">)</mo></math> of the <math display="inline"><mrow><mi>χ</mi><mi>SF</mi></mrow></math> valence action, in order to ensure that QCD symmetries are fully recovered in the continuum. The properties of this novel setup are monitored through the ratios <math display="inline"><msub><mi>Z</mi><mi>S</mi></msub><mo>/</mo><msub><mi>Z</mi><mi>P</mi></msub></math> and <math display="inline"><msub><mi mathvariant="normal">Σ</mi><mi>S</mi></msub><mo>/</mo><msub><mi mathvariant="normal">Σ</mi><mi>P</mi></msub></math> of the renormalization parameters and step scaling functions of the scalar and pseudoscalar densities. Where comparison is possible, our <math display="inline"><msub><mi>Z</mi><mi>S</mi></msub><mo>/</mo><msub><mi>Z</mi><mi>P</mi></msub></math> results are found to agree with previous determinations, based on a mass ratio method [G. M. de Divitiis (ALPHA Collaboration), Eur. Phys. J. C 79, 797 (2019)] and Ward identities [ J. Heitger (ALPHA Collaboration), Eur. Phys. J. C 80, 765 (2020); J. Heitger , Eur. Phys. J. C 81, 606 (2021)], with Schrödinger functional boundary conditions. The behavior of <math display="inline"><msub><mi mathvariant="normal">Σ</mi><mi>S</mi></msub><mo>/</mo><msub><mi mathvariant="normal">Σ</mi><mi>P</mi></msub></math> confirms the theoretical expectations of <math display="inline"><mrow><mi>χ</mi><mi>SF</mi></mrow></math> QCD, related to the restoration of the theory’s symmetries in the continuum limit. From the step-scaling function of the pseudoscalar density we obtain the quark mass RG-running function from hadronic to perturbative energy scales. This is fully compatible with the earlier result obtained in a similar setup for Wilson quarks with Schrödinger functional boundary conditions [I. Campos , Eur. Phys. J. C 78, 387 (2018)], and provides a strong universality test for the two lattice setups.We study the Renormalisation Group (RG) running of the quark mass, for $N_f=3$ QCD with Wilson fermions in a mixed action setup, with standard Schrödinger Functional (SF) boundary conditions for sea quarks and chirally rotated Schrödinger Functional ($\chi$SF) boundary conditions for valence quarks. This necessitates the tuning of the boundary factor $z_f(g_0^2)$ of the $\chi$SF valence action, in order to ensure that QCD symmetries are fully recovered in the continuum. The properties of this novel setup are monitored through the ratios $Z_S/Z_P$ and $\Sigma_S/\Sigma_P$ of the renormalisation parameters and step scaling functions of the scalar and pseudoscalar densities. Where comparison is possible, our $Z_S/Z_P$ results are found to agree with previous determinations, based on a mass ratio method arXiv:1906.03445 and Ward identities arXiv:2005.01352, arXiv:2101.10969, with Schrödinger Functional boundary conditions. The behaviour of $\Sigma_S/\Sigma_P$ confirms the theoretical expectations of $\chi$SF QCD, related to the restoration of the theory's symmetries in the continuum limit. From the step scaling function of the pseudoscalar density we obtain the quark mass RG-running function from hadronic to perturbative energy scales. This is fully compatible with the earlier result obtained in a similar setup for Wilson quarks with Schrödinger Functional boundary conditions arXiv:1802.05243 and provides a strong universality test for the two lattice setups.arXiv:2112.10606oai:cds.cern.ch:27985782021-12-20
spellingShingle hep-lat
Particle Physics - Lattice
Plasencia, Isabel Campos
Brida, Mattia Dalla
de Divitiis, Giulia Maria
Lytle, Andrew
Papinutto, Mauro
Pirelli, Ludovica
Vladikas, Anastassios
Nonperturbative running of the quark mass for $N$$_{f}$ = 3 QCD from the chirally rotated Schrödinger functional
title Nonperturbative running of the quark mass for $N$$_{f}$ = 3 QCD from the chirally rotated Schrödinger functional
title_full Nonperturbative running of the quark mass for $N$$_{f}$ = 3 QCD from the chirally rotated Schrödinger functional
title_fullStr Nonperturbative running of the quark mass for $N$$_{f}$ = 3 QCD from the chirally rotated Schrödinger functional
title_full_unstemmed Nonperturbative running of the quark mass for $N$$_{f}$ = 3 QCD from the chirally rotated Schrödinger functional
title_short Nonperturbative running of the quark mass for $N$$_{f}$ = 3 QCD from the chirally rotated Schrödinger functional
title_sort nonperturbative running of the quark mass for $n$$_{f}$ = 3 qcd from the chirally rotated schrödinger functional
topic hep-lat
Particle Physics - Lattice
url https://dx.doi.org/10.1103/PhysRevD.105.054506
http://cds.cern.ch/record/2798578
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