Parton physics from a heavy-quark operator product expansion: Lattice QCD calculation of the fourth moment of the pion distribution amplitude

The pion light-cone distribution amplitude (LCDA) is an essential nonperturbative input for a range of high-energy exclusive processes in quantum chromodynamics. Building on our previous work, the continuum limit of the fourth Mellin moment of the pion LCDA is determined in quenched QCD using quark masses which correspond to a pion mass of <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:msub> <a:mi>m</a:mi> <a:mi>π</a:mi> </a:msub> <a:mo>=</a:mo> <a:mn>550</a:mn> <a:mtext> </a:mtext> <a:mtext> </a:mtext> <a:mi>MeV</a:mi> </a:math> . This calculation finds <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"> <c:mrow> <c:mo stretchy="false">⟨</c:mo> <c:msup> <c:mrow> <c:mi>ξ</c:mi> </c:mrow> <c:mrow> <c:mn>2</c:mn> </c:mrow> </c:msup> <c:mo stretchy="false">⟩</c:mo> <c:mo>=</c:mo> <c:mn>0.202</c:mn> <c:mo stretchy="false">(</c:mo> <c:mn>8</c:mn> <c:mo stretchy="false">)</c:mo> <c:mo stretchy="false">(</c:mo> <c:mn>9</c:mn> <c:mo stretchy="false">)</c:mo> </c:mrow> </c:math> and <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"> <k:mrow> <k:mo stretchy="false">⟨</k:mo> <k:msup> <k:mrow> <k:mi>ξ</k:mi> </k:mrow> <k:mrow> <k:mn>4</k:mn> </k:mrow> </k:msup> <k:mo stretchy="false">⟩</k:mo> <k:mo>=</k:mo> <k:mn>0.039</k:mn> <k:mo stretchy="false">(</k:mo> <k:mn>28</k:mn> <k:mo stretchy="false">)</k:mo> <k:mo stretchy="false">(</k:mo> <k:mn>11</k:mn> <k:mo stretchy="false">)</k:mo> </k:mrow> </k:math> where the first error indicates the combined statistical and systematic uncertainty from the analysis and the second indicates the uncertainty from working with Wilson coefficients computed to next-to-leading order. These results are presented in the <s:math xmlns:s="http://www.w3.org/1998/Math/MathML" display="inline"> <s:mover accent="true"> <s:mrow> <s:mi>MS</s:mi> </s:mrow> <s:mo stretchy="true">¯</s:mo> </s:mover> </s:math> scheme at a renormalization scale of <w:math xmlns:w="http://www.w3.org/1998/Math/MathML" display="inline"> <w:mrow> <w:mi>μ</w:mi> <w:mo>=</w:mo> <w:mn>2</w:mn> <w:mtext> </w:mtext> <w:mtext> </w:mtext> <w:mi>GeV</w:mi> </w:mrow> </w:math> .

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Journal
Physical review. D/Physical review. D.
Published
2025-12-17
DOI
https://doi.org/10.1103/xs4z-nblq
Citations
2
Primary Topic
Quantum Chromodynamics and Particle Interactions
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article
Field-Weighted Citation Impact
3.74
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article

Parton physics from a heavy-quark operator product expansion: Lattice QCD calculation of the fourth moment of the pion distribution amplitude

Karl J. Friston
2 citations
Physical review. D/Physical review. D.
Quantum Chromodynamics and Particle Interactions
3.74
article

Parton physics from a heavy-quark operator product expansion: Lattice QCD calculation of the fourth moment of the pion distribution amplitude

Karl J. Friston
article en
2 citations

Abstract

The pion light-cone distribution amplitude (LCDA) is an essential nonperturbative input for a range of high-energy exclusive processes in quantum chromodynamics. Building on our previous work, the continuum limit of the fourth Mellin moment of the pion LCDA is determined in quenched QCD using quark masses which correspond to a pion mass of <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:msub> <a:mi>m</a:mi> <a:mi>π</a:mi> </a:msub> <a:mo>=</a:mo> <a:mn>550</a:mn> <a:mtext> </a:mtext> <a:mtext> </a:mtext> <a:mi>MeV</a:mi> </a:math> . This calculation finds <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"> <c:mrow> <c:mo stretchy="false">⟨</c:mo> <c:msup> <c:mrow> <c:mi>ξ</c:mi> </c:mrow> <c:mrow> <c:mn>2</c:mn> </c:mrow> </c:msup> <c:mo stretchy="false">⟩</c:mo> <c:mo>=</c:mo> <c:mn>0.202</c:mn> <c:mo stretchy="false">(</c:mo> <c:mn>8</c:mn> <c:mo stretchy="false">)</c:mo> <c:mo stretchy="false">(</c:mo> <c:mn>9</c:mn> <c:mo stretchy="false">)</c:mo> </c:mrow> </c:math> and <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"> <k:mrow> <k:mo stretchy="false">⟨</k:mo> <k:msup> <k:mrow> <k:mi>ξ</k:mi> </k:mrow> <k:mrow> <k:mn>4</k:mn> </k:mrow> </k:msup> <k:mo stretchy="false">⟩</k:mo> <k:mo>=</k:mo> <k:mn>0.039</k:mn> <k:mo stretchy="false">(</k:mo> <k:mn>28</k:mn> <k:mo stretchy="false">)</k:mo> <k:mo stretchy="false">(</k:mo> <k:mn>11</k:mn> <k:mo stretchy="false">)</k:mo> </k:mrow> </k:math> where the first error indicates the combined statistical and systematic uncertainty from the analysis and the second indicates the uncertainty from working with Wilson coefficients computed to next-to-leading order. These results are presented in the <s:math xmlns:s="http://www.w3.org/1998/Math/MathML" display="inline"> <s:mover accent="true"> <s:mrow> <s:mi>MS</s:mi> </s:mrow> <s:mo stretchy="true">¯</s:mo> </s:mover> </s:math> scheme at a renormalization scale of <w:math xmlns:w="http://www.w3.org/1998/Math/MathML" display="inline"> <w:mrow> <w:mi>μ</w:mi> <w:mo>=</w:mo> <w:mn>2</w:mn> <w:mtext> </w:mtext> <w:mtext> </w:mtext> <w:mi>GeV</w:mi> </w:mrow> </w:math> .

Physical review. D/Physical review. D.Vol. 113(1)
Argonne National Laboratory (US), Fermi National Accelerator Laboratory (US), National Yang Ming Chiao Tung University (TW), Chung Yuan Christian University (TW), RIKEN Center for Computational Science (JP), Massachusetts Institute of Technology (US)
Openalex Percentile: Top 6%
Quantum Chromodynamics and Particle Interactions
3.74
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