Hadronic light-by-light contribution to the muon anomaly from lattice QCD with infinite volume QED at physical pion mass

The hadronic light-by-light scattering contribution to the muon anomalous magnetic moment, <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mrow><a:mo stretchy="false">(</a:mo><a:mi>g</a:mi><a:mo>−</a:mo><a:mn>2</a:mn><a:mo stretchy="false">)</a:mo><a:mrow><a:mo>/</a:mo><a:mn>2</a:mn></a:mrow></a:mrow></a:math>, is computed in the infinite volume QED framework with lattice QCD. We report <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:msubsup><e:mi>a</e:mi><e:mi>μ</e:mi><e:mtext>HLbL</e:mtext></e:msubsup><e:mo>=</e:mo><e:mn>12.47</e:mn><e:mo stretchy="false">(</e:mo><e:mn>1.15</e:mn><e:mo stretchy="false">)</e:mo><e:mo stretchy="false">(</e:mo><e:mn>0.95</e:mn><e:mo stretchy="false">)</e:mo><e:mo>×</e:mo><e:msup><e:mn>10</e:mn><e:mrow><e:mo>−</e:mo><e:mn>10</e:mn></e:mrow></e:msup></e:math> where the first error is statistical and the second systematic. The result is mainly based on the <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"><k:mrow><k:mn>2</k:mn><k:mo>+</k:mo><k:mn>1</k:mn></k:mrow></k:math> flavor Möbius domain wall fermion ensemble with inverse lattice spacing <m:math xmlns:m="http://www.w3.org/1998/Math/MathML" display="inline"><m:msup><m:mi>a</m:mi><m:mrow><m:mo>−</m:mo><m:mn>1</m:mn></m:mrow></m:msup><m:mo>=</m:mo><m:mn>1.73</m:mn><m:mtext> </m:mtext><m:mtext> </m:mtext><m:mi>GeV</m:mi></m:math>, lattice size <o:math xmlns:o="http://www.w3.org/1998/Math/MathML" display="inline"><o:mi>L</o:mi><o:mo>=</o:mo><o:mn>5.5</o:mn><o:mtext> </o:mtext><o:mtext> </o:mtext><o:mi>fm</o:mi></o:math>, and <q:math xmlns:q="http://www.w3.org/1998/Math/MathML" display="inline"><q:msub><q:mi>m</q:mi><q:mi>π</q:mi></q:msub><q:mo>=</q:mo><q:mn>139</q:mn><q:mtext> </q:mtext><q:mtext> </q:mtext><q:mi>MeV</q:mi></q:math>, generated by the RBC-UKQCD collaborations. The leading systematic error of this result comes from the lattice discretization. This result is consistent with previous determinations.

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Publication Details

Journal
Physical review. D/Physical review. D.
Published
2025-01-10
DOI
https://doi.org/10.1103/physrevd.111.014501
Citations
23
Primary Topic
Quantum Chromodynamics and Particle Interactions
Type
article
Field-Weighted Citation Impact
43.01

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article

Hadronic light-by-light contribution to the muon anomaly from lattice QCD with infinite volume QED at physical pion mass

Masashi Hayakawa, Cheng Tu, Taku Izubuchi, Thomas Blum et al.
23 citations
Physical review. D/Physical review. D.
Quantum Chromodynamics and Particle Interactions
43.01
article

Hadronic light-by-light contribution to the muon anomaly from lattice QCD with infinite volume QED at physical pion mass

Masashi Hayakawa, Cheng Tu, Taku Izubuchi, Thomas Blum, Chulwoo Jung, Luchang Jin, Norman H. Christ, Christoph Lehner
article en
23 citations

Abstract

The hadronic light-by-light scattering contribution to the muon anomalous magnetic moment, <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mrow><a:mo stretchy="false">(</a:mo><a:mi>g</a:mi><a:mo>−</a:mo><a:mn>2</a:mn><a:mo stretchy="false">)</a:mo><a:mrow><a:mo>/</a:mo><a:mn>2</a:mn></a:mrow></a:mrow></a:math>, is computed in the infinite volume QED framework with lattice QCD. We report <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:msubsup><e:mi>a</e:mi><e:mi>μ</e:mi><e:mtext>HLbL</e:mtext></e:msubsup><e:mo>=</e:mo><e:mn>12.47</e:mn><e:mo stretchy="false">(</e:mo><e:mn>1.15</e:mn><e:mo stretchy="false">)</e:mo><e:mo stretchy="false">(</e:mo><e:mn>0.95</e:mn><e:mo stretchy="false">)</e:mo><e:mo>×</e:mo><e:msup><e:mn>10</e:mn><e:mrow><e:mo>−</e:mo><e:mn>10</e:mn></e:mrow></e:msup></e:math> where the first error is statistical and the second systematic. The result is mainly based on the <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"><k:mrow><k:mn>2</k:mn><k:mo>+</k:mo><k:mn>1</k:mn></k:mrow></k:math> flavor Möbius domain wall fermion ensemble with inverse lattice spacing <m:math xmlns:m="http://www.w3.org/1998/Math/MathML" display="inline"><m:msup><m:mi>a</m:mi><m:mrow><m:mo>−</m:mo><m:mn>1</m:mn></m:mrow></m:msup><m:mo>=</m:mo><m:mn>1.73</m:mn><m:mtext> </m:mtext><m:mtext> </m:mtext><m:mi>GeV</m:mi></m:math>, lattice size <o:math xmlns:o="http://www.w3.org/1998/Math/MathML" display="inline"><o:mi>L</o:mi><o:mo>=</o:mo><o:mn>5.5</o:mn><o:mtext> </o:mtext><o:mtext> </o:mtext><o:mi>fm</o:mi></o:math>, and <q:math xmlns:q="http://www.w3.org/1998/Math/MathML" display="inline"><q:msub><q:mi>m</q:mi><q:mi>π</q:mi></q:msub><q:mo>=</q:mo><q:mn>139</q:mn><q:mtext> </q:mtext><q:mtext> </q:mtext><q:mi>MeV</q:mi></q:math>, generated by the RBC-UKQCD collaborations. The leading systematic error of this result comes from the lattice discretization. This result is consistent with previous determinations.

Physical review. D/Physical review. D.Vol. 111(1)
Brookhaven National Laboratory (US), RIKEN (JP), Nagoya University (JP), University of Regensburg (DE), Columbia University (US)
U.S. Department of Energy, Office of Science, Japan Society for the Promotion of Science, RIKEN, Laboratory Directed Research and Development
Openalex Percentile: Top 0%
Quantum Chromodynamics and Particle Interactions
43.01
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