Determination of heavy meson light-cone distribution amplitudes: theoretical framework and lattice simulations

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Main Authors: Gao, Hao-Fei, Han, Xue-Ying, Hua, Jun, Ji, Xiangdong, Jiang, Xiangyu, Lü, Cai-Dian, Schäfer, Andreas, Jin-XinTan, Wang, Ji-Hao, Wang, Wei, Xu, Ji, Yang, Yi-Bo, Zhang, Fu-Wei, Zhang, Jian-Hui, Zhang, Jia-Lu, Zhang, Mu-Hua, Zhang, Qi-An, Zhao, Shuai
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Published: 2026
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author Gao, Hao-Fei
Han, Xue-Ying
Hua, Jun
Ji, Xiangdong
Jiang, Xiangyu
Lü, Cai-Dian
Schäfer, Andreas
Jin-XinTan
Wang, Ji-Hao
Wang, Wei
Xu, Ji
Yang, Yi-Bo
Zhang, Fu-Wei
Zhang, Jian-Hui
Zhang, Jia-Lu
Zhang, Mu-Hua
Zhang, Qi-An
Zhao, Shuai
author_facet Gao, Hao-Fei
Han, Xue-Ying
Hua, Jun
Ji, Xiangdong
Jiang, Xiangyu
Lü, Cai-Dian
Schäfer, Andreas
Jin-XinTan
Wang, Ji-Hao
Wang, Wei
Xu, Ji
Yang, Yi-Bo
Zhang, Fu-Wei
Zhang, Jian-Hui
Zhang, Jia-Lu
Zhang, Mu-Hua
Zhang, Qi-An
Zhao, Shuai
contents We present a first-principles determination of heavy meson light-cone distribution amplitudes (LCDAs) from lattice QCD in the continuum limit, improving substantially on our previous pioneering study. Within the heavy-quark large-momentum effective theory (HQLaMET) framework, supplemented by lattice QCD calculations of the OPE moments, we analyze six ensembles with lattice spacings ranging from $a=0.0519-0.1053$\,fm and pion masses from $m_π=135.5-317.2$\,MeV, thereby enabling controlled continuum, chiral, and infinite-momentum extrapolations to the physical point. Momentum-smeared sources, hypercubic-smeared Wilson lines, and optimized interpolating operators are adopted to significantly improved signals for the nonlocal correlators. Within a unified framework, we determine both QCD LCDAs and HQET LCDAs. Our resulting QCD LCDAs of $D$ meson peak at $y\approx 0.2-0.3$, with total uncertainties below $30\%$ for $0.1<y<0.9$. The leading-twist HQET LCDA is constructed using a peak-and-tail factorization, in which the nonperturbative peak region is obtained from lattice QCD and the perturbative tail is incorporated from HQET, with the two regions combined through a model-independent Laguerre-polynomial parametrization. At $μ=1$\,GeV, we obtain the inverse moment of HQET LCDA $λ_B=0.340(20)$\,GeV and first inverse-logarithmic moment $σ_B^{(1)}=1.685(63)$, consistent with experimental constraints and phenomenological determinations. Direct lattice calculations based on operator product expansion provide a nontrivial cross-check of the LaMET results. Final results and phenomenological impact of these results are presented in a companion paper~\cite{HeavymesonDA_short_paper}. Our results remove the single-lattice-spacing limitation of the previous study, and provide a robust determinations of heavy meson LCDAs in both QCD and HQET for next-generation heavy flavor physics.
format Preprint
id arxiv_https___arxiv_org_abs_2604_25802
institution arXiv
publishDate 2026
record_format arxiv
spellingShingle Determination of heavy meson light-cone distribution amplitudes: theoretical framework and lattice simulations
Gao, Hao-Fei
Han, Xue-Ying
Hua, Jun
Ji, Xiangdong
Jiang, Xiangyu
Lü, Cai-Dian
Schäfer, Andreas
Jin-XinTan
Wang, Ji-Hao
Wang, Wei
Xu, Ji
Yang, Yi-Bo
Zhang, Fu-Wei
Zhang, Jian-Hui
Zhang, Jia-Lu
Zhang, Mu-Hua
Zhang, Qi-An
Zhao, Shuai
High Energy Physics - Lattice
We present a first-principles determination of heavy meson light-cone distribution amplitudes (LCDAs) from lattice QCD in the continuum limit, improving substantially on our previous pioneering study. Within the heavy-quark large-momentum effective theory (HQLaMET) framework, supplemented by lattice QCD calculations of the OPE moments, we analyze six ensembles with lattice spacings ranging from $a=0.0519-0.1053$\,fm and pion masses from $m_π=135.5-317.2$\,MeV, thereby enabling controlled continuum, chiral, and infinite-momentum extrapolations to the physical point. Momentum-smeared sources, hypercubic-smeared Wilson lines, and optimized interpolating operators are adopted to significantly improved signals for the nonlocal correlators. Within a unified framework, we determine both QCD LCDAs and HQET LCDAs. Our resulting QCD LCDAs of $D$ meson peak at $y\approx 0.2-0.3$, with total uncertainties below $30\%$ for $0.1<y<0.9$. The leading-twist HQET LCDA is constructed using a peak-and-tail factorization, in which the nonperturbative peak region is obtained from lattice QCD and the perturbative tail is incorporated from HQET, with the two regions combined through a model-independent Laguerre-polynomial parametrization. At $μ=1$\,GeV, we obtain the inverse moment of HQET LCDA $λ_B=0.340(20)$\,GeV and first inverse-logarithmic moment $σ_B^{(1)}=1.685(63)$, consistent with experimental constraints and phenomenological determinations. Direct lattice calculations based on operator product expansion provide a nontrivial cross-check of the LaMET results. Final results and phenomenological impact of these results are presented in a companion paper~\cite{HeavymesonDA_short_paper}. Our results remove the single-lattice-spacing limitation of the previous study, and provide a robust determinations of heavy meson LCDAs in both QCD and HQET for next-generation heavy flavor physics.
title Determination of heavy meson light-cone distribution amplitudes: theoretical framework and lattice simulations
topic High Energy Physics - Lattice
url https://arxiv.org/abs/2604.25802