Matching the quasiparton distribution in a momentum subtraction scheme

The quasiparton distribution is a spatial correlation of quarks or gluons along the z direction in a moving nucleon which enables direct lattice calculations of parton distribution functions. It can be defined with a nonperturbative renormalization in a regularization independent momentum subtractio...

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Bibliographic Details
Main Authors: Stewart, Iain W (Contributor), Zhao, Yong (Contributor)
Other Authors: Massachusetts Institute of Technology. Center for Theoretical Physics (Contributor), Massachusetts Institute of Technology. Department of Physics (Contributor), Massachusetts Institute of Technology. Laboratory for Nuclear Science (Contributor)
Format: Article
Language:English
Published: American Physical Society, 2018-04-04T16:20:21Z.
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Online Access:Get fulltext
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042 |a dc 
100 1 0 |a Stewart, Iain W  |e author 
100 1 0 |a Massachusetts Institute of Technology. Center for Theoretical Physics  |e contributor 
100 1 0 |a Massachusetts Institute of Technology. Department of Physics  |e contributor 
100 1 0 |a Massachusetts Institute of Technology. Laboratory for Nuclear Science  |e contributor 
100 1 0 |a Stewart, Iain W  |e contributor 
100 1 0 |a Zhao, Yong  |e contributor 
700 1 0 |a Zhao, Yong  |e author 
245 0 0 |a Matching the quasiparton distribution in a momentum subtraction scheme 
260 |b American Physical Society,   |c 2018-04-04T16:20:21Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/114541 
520 |a The quasiparton distribution is a spatial correlation of quarks or gluons along the z direction in a moving nucleon which enables direct lattice calculations of parton distribution functions. It can be defined with a nonperturbative renormalization in a regularization independent momentum subtraction scheme (RI/MOM), which can then be perturbatively related to the collinear parton distribution in the MS[over ¯] scheme. Here we carry out a direct matching from the RI/MOM scheme for the quasi-PDF to the MS[over ¯] PDF, determining the non-singlet quark matching coefficient at next-to-leading order in perturbation theory. We find that the RI/MOM matching coefficient is insensitive to the ultraviolet region of convolution integral, exhibits improved perturbative convergence when converting between the quasi-PDF and PDF, and is consistent with a quasi-PDF that vanishes in the unphysical region as the proton momentum P[superscript z]→∞, unlike other schemes. This direct approach therefore has the potential to improve the accuracy for converting quasidistribution lattice calculations to collinear distributions. 
520 |a United States. Department of Energy (Grant DE-SC0011090) 
520 |a Simons Foundation (Grant 327942) 
546 |a en 
655 7 |a Article 
773 |t Physical Review D