Transverse-momentum-dependent pion structures from lattice QCD: Collins-Soper kernel, soft factor, TMDWF, and TMDPDF

We present the first lattice quantum chromodynamics (QCD) calculation of the pion valence-quark transverse-momentum-dependent parton distribution function (TMDPDF) within the framework of large-momentum effective theory (LaMET). Using correlators fixed in the Coulomb gauge (CG), we computed the quasi-TMD beam function for a pion with a mass of 300 MeV, a fine lattice spacing of <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mi>a</a:mi><a:mo>=</a:mo><a:mn>0.06</a:mn><a:mtext> </a:mtext><a:mtext> </a:mtext><a:mi>fm</a:mi></a:math>, and multiple large momenta up to 3 GeV. The intrinsic soft functions in the CG approach are extracted from form factors with large momentum transfer, and as a byproduct, we also obtain the corresponding Collins-Soper (CS) kernel. Our determinations of both the soft function and the CS kernel agree with perturbation theory at small transverse separations (<c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:msub><c:mi>b</c:mi><c:mo>⊥</c:mo></c:msub></c:math>) between the quarks. At larger <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:msub><e:mi>b</e:mi><e:mo>⊥</e:mo></e:msub></e:math>, the CS kernel remains consistent with recent results obtained using both CG and gauge-invariant TMD correlators in the literature. By combining next-to-leading logarithmic factorization of the quasi-TMD beam function and the soft function, we obtain an <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"><g:mi>x</g:mi></g:math>-dependent pion valence-quark TMDPDF for transverse separations <i:math xmlns:i="http://www.w3.org/1998/Math/MathML" display="inline"><i:msub><i:mi>b</i:mi><i:mo>⊥</i:mo></i:msub><i:mo>≳</i:mo><i:mn>1</i:mn><i:mtext> </i:mtext><i:mtext> </i:mtext><i:mi>fm</i:mi></i:math>. Interestingly, we find that the <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"><k:msub><k:mi>b</k:mi><k:mo>⊥</k:mo></k:msub></k:math> dependence of the phenomenological parametrizations of TMDPDF for moderate values of <m:math xmlns:m="http://www.w3.org/1998/Math/MathML" display="inline"><m:mi>x</m:mi></m:math> are in reasonable agreement with our QCD determinations. In addition, we present results for the transverse-momentum-dependent wave function for a heavier pion with 670 MeV mass.

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Journal
Physical review. D/Physical review. D.
Published
2025-07-14
DOI
https://doi.org/10.1103/j3n6-8kxy
Citations
9
Primary Topic
Quantum Chromodynamics and Particle Interactions
Type
article
Field-Weighted Citation Impact
16.83

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article

Transverse-momentum-dependent pion structures from lattice QCD: Collins-Soper kernel, soft factor, TMDWF, and TMDPDF

Yong Zhao, Xiang Gao, Jin-Chen He, Swagato Mukherjee et al.
9 citations
Physical review. D/Physical review. D.
Quantum Chromodynamics and Particle Interactions
16.83
article

Transverse-momentum-dependent pion structures from lattice QCD: Collins-Soper kernel, soft factor, TMDWF, and TMDPDF

Yong Zhao, Xiang Gao, Jin-Chen He, Swagato Mukherjee, Karl J. Friston
article en
9 citations

Abstract

We present the first lattice quantum chromodynamics (QCD) calculation of the pion valence-quark transverse-momentum-dependent parton distribution function (TMDPDF) within the framework of large-momentum effective theory (LaMET). Using correlators fixed in the Coulomb gauge (CG), we computed the quasi-TMD beam function for a pion with a mass of 300 MeV, a fine lattice spacing of <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mi>a</a:mi><a:mo>=</a:mo><a:mn>0.06</a:mn><a:mtext> </a:mtext><a:mtext> </a:mtext><a:mi>fm</a:mi></a:math>, and multiple large momenta up to 3 GeV. The intrinsic soft functions in the CG approach are extracted from form factors with large momentum transfer, and as a byproduct, we also obtain the corresponding Collins-Soper (CS) kernel. Our determinations of both the soft function and the CS kernel agree with perturbation theory at small transverse separations (<c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:msub><c:mi>b</c:mi><c:mo>⊥</c:mo></c:msub></c:math>) between the quarks. At larger <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:msub><e:mi>b</e:mi><e:mo>⊥</e:mo></e:msub></e:math>, the CS kernel remains consistent with recent results obtained using both CG and gauge-invariant TMD correlators in the literature. By combining next-to-leading logarithmic factorization of the quasi-TMD beam function and the soft function, we obtain an <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"><g:mi>x</g:mi></g:math>-dependent pion valence-quark TMDPDF for transverse separations <i:math xmlns:i="http://www.w3.org/1998/Math/MathML" display="inline"><i:msub><i:mi>b</i:mi><i:mo>⊥</i:mo></i:msub><i:mo>≳</i:mo><i:mn>1</i:mn><i:mtext> </i:mtext><i:mtext> </i:mtext><i:mi>fm</i:mi></i:math>. Interestingly, we find that the <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"><k:msub><k:mi>b</k:mi><k:mo>⊥</k:mo></k:msub></k:math> dependence of the phenomenological parametrizations of TMDPDF for moderate values of <m:math xmlns:m="http://www.w3.org/1998/Math/MathML" display="inline"><m:mi>x</m:mi></m:math> are in reasonable agreement with our QCD determinations. In addition, we present results for the transverse-momentum-dependent wave function for a heavier pion with 670 MeV mass.

Physical review. D/Physical review. D.Vol. 112(3)
Argonne National Laboratory (US), Brookhaven National Laboratory (US), University of Maryland, College Park (US)
U.S. Department of Energy, National Energy Research Scientific Computing Center, Office of Science, Nuclear Physics, Laboratory Directed Research and Development, Argonne National Laboratory
Openalex Percentile: Top 1%
Quantum Chromodynamics and Particle Interactions
16.83
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