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A Hybrid Renormalization Scheme for Quasi Light-Front Correlations in Large-Momentum Effective Theory

High Energy Physics - Phenomenology 2021-01-20 v2 High Energy Physics - Experiment High Energy Physics - Lattice Nuclear Experiment Nuclear Theory

Abstract

In large-momentum effective theory (LaMET), calculating parton physics starts from calculating coordinate-space-zz correlation functions h~(z,a,Pz)\tilde h(z, a,P^z) in a hadron of momentum PzP^z in lattice QCD. Such correlation functions involve both linear and logarithmic divergences in lattice spacing aa, and thus need to be properly renormalized. We introduce a hybrid renormalization procedure to match these lattice correlations to those in the continuum MS\overline{\rm MS} scheme, without introducing extra non-perturbative effects at large zz. We analyze the effect of O(ΛQCD){\cal O}(\Lambda_{\rm QCD}) ambiguity in the Wilson line self-energy subtraction involved in this hybrid scheme. To obtain the momentum-space distributions, we recommend to extrapolate the lattice data to the asymptotic zz-region using the generic properties of the coordinate space correlations at moderate and large PzP^z, respectively.

Keywords

Cite

@article{arxiv.2008.03886,
  title  = {A Hybrid Renormalization Scheme for Quasi Light-Front Correlations in Large-Momentum Effective Theory},
  author = {Xiangdong Ji and Yizhuang Liu and Andreas Schäfer and Wei Wang and Yi-Bo Yang and Jian-Hui Zhang and Yong Zhao},
  journal= {arXiv preprint arXiv:2008.03886},
  year   = {2021}
}

Comments

Text revised, version to appear in NPB