Lattice QCD calculation of the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>η</mml:mi></mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi

We present a lattice calculation of the <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mi>η</a:mi></a:math> and <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:msup><c:mi>η</c:mi><c:mo>′</c:mo></c:msup></c:math> meson masses at the physical point and in the continuum limit, based on <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:msub><e:mi>N</e:mi><e:mi>f</e:mi></e:msub><e:mo>=</e:mo><e:mn>2</e:mn><e:mo>+</e:mo><e:mn>1</e:mn><e:mo>+</e:mo><e:mn>1</e:mn></e:math> flavors of rooted staggered quarks. Our analysis includes gauge ensembles at the physical pion and kaon masses spread over six lattice spacings in the range [0.064–0.1315] fm. Our main results read <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"><g:msub><g:mi>m</g:mi><g:mi>η</g:mi></g:msub><g:mo>=</g:mo><g:mn>543.5</g:mn><g:mo stretchy="false">(</g:mo><g:mn>5.6</g:mn><g:mo stretchy="false">)</g:mo><g:mtext> </g:mtext><g:mtext> </g:mtext><g:mi>MeV</g:mi></g:math> and <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"><k:msub><k:mi>m</k:mi><k:msup><k:mi>η</k:mi><k:mo>′</k:mo></k:msup></k:msub><k:mo>=</k:mo><k:mn>986</k:mn><k:mo stretchy="false">(</k:mo><k:mn>38</k:mn><k:mo stretchy="false">)</k:mo><k:mtext> </k:mtext><k:mtext> </k:mtext><k:mi>MeV</k:mi></k:math>, consistent with the experimental values. This is an important numerical test that supports the validity of the fourth root procedure used in the staggered quark formalism. This calculation was the first step toward extracting the pseudoscalar transition form factors of the <o:math xmlns:o="http://www.w3.org/1998/Math/MathML" display="inline"><o:mi>η</o:mi></o:math> and <q:math xmlns:q="http://www.w3.org/1998/Math/MathML" display="inline"><q:msup><q:mi>η</q:mi><q:mo>′</q:mo></q:msup></q:math> mesons that play a crucial role in the hadronic light-by-light contribution to the muon <s:math xmlns:s="http://www.w3.org/1998/Math/MathML" display="inline"><s:mi>g</s:mi><s:mo>−</s:mo><s:mn>2</s:mn></s:math>.

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Publication Details

Journal
Physical review. D/Physical review. D.
Published
2025-05-07
DOI
https://doi.org/10.1103/physrevd.111.094506
Citations
3
Primary Topic
Quantum Chromodynamics and Particle Interactions
Type
article
Field-Weighted Citation Impact
5.61

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article

Lattice QCD calculation of the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>η</mml:mi></mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi

Jana N. Guenther, Willem E. A. Verplanke, Z. Fodor, Lukas Varnhorst et al.
3 citations
Physical review. D/Physical review. D.
Quantum Chromodynamics and Particle Interactions
5.61
article

Lattice QCD calculation of the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>η</mml:mi></mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi

Jana N. Guenther, Willem E. A. Verplanke, Z. Fodor, Lukas Varnhorst, Antoine Gérardin, Laurent Lellouch, Bálint Tóth, Kálman Szabó
article en
3 citations

Abstract

We present a lattice calculation of the <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mi>η</a:mi></a:math> and <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:msup><c:mi>η</c:mi><c:mo>′</c:mo></c:msup></c:math> meson masses at the physical point and in the continuum limit, based on <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:msub><e:mi>N</e:mi><e:mi>f</e:mi></e:msub><e:mo>=</e:mo><e:mn>2</e:mn><e:mo>+</e:mo><e:mn>1</e:mn><e:mo>+</e:mo><e:mn>1</e:mn></e:math> flavors of rooted staggered quarks. Our analysis includes gauge ensembles at the physical pion and kaon masses spread over six lattice spacings in the range [0.064–0.1315] fm. Our main results read <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"><g:msub><g:mi>m</g:mi><g:mi>η</g:mi></g:msub><g:mo>=</g:mo><g:mn>543.5</g:mn><g:mo stretchy="false">(</g:mo><g:mn>5.6</g:mn><g:mo stretchy="false">)</g:mo><g:mtext> </g:mtext><g:mtext> </g:mtext><g:mi>MeV</g:mi></g:math> and <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"><k:msub><k:mi>m</k:mi><k:msup><k:mi>η</k:mi><k:mo>′</k:mo></k:msup></k:msub><k:mo>=</k:mo><k:mn>986</k:mn><k:mo stretchy="false">(</k:mo><k:mn>38</k:mn><k:mo stretchy="false">)</k:mo><k:mtext> </k:mtext><k:mtext> </k:mtext><k:mi>MeV</k:mi></k:math>, consistent with the experimental values. This is an important numerical test that supports the validity of the fourth root procedure used in the staggered quark formalism. This calculation was the first step toward extracting the pseudoscalar transition form factors of the <o:math xmlns:o="http://www.w3.org/1998/Math/MathML" display="inline"><o:mi>η</o:mi></o:math> and <q:math xmlns:q="http://www.w3.org/1998/Math/MathML" display="inline"><q:msup><q:mi>η</q:mi><q:mo>′</q:mo></q:msup></q:math> mesons that play a crucial role in the hadronic light-by-light contribution to the muon <s:math xmlns:s="http://www.w3.org/1998/Math/MathML" display="inline"><s:mi>g</s:mi><s:mo>−</s:mo><s:mn>2</s:mn></s:math>.

Physical review. D/Physical review. D.Vol. 111(9)
Eötvös Loránd University (HU), Pennsylvania State University (US), Université de Toulon (FR), University of Wuppertal (DE), Forschungszentrum Jülich (DE), Aix-Marseille Université (FR), Center for Pastor Theologians (US)
Aix-Marseille Université, Agence Nationale de la Recherche, Forschungszentrum Jülich, Grand Équipement National De Calcul Intensif, Gauss Centre for Supercomputing, Leibniz-Gemeinschaft, Leibniz-Rechenzentrum
Openalex Percentile: Top 5%
Quantum Chromodynamics and Particle Interactions
5.61
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