Quark orbital angular momentum as a chiral magnetic effect

Fuente: arXiv
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Hauptverfasser: Kim, June-Young, Won, Ho-Yeon, Weiss, Christian
Format: Preprint
Veröffentlicht: 2026
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author Kim, June-Young
Won, Ho-Yeon
Weiss, Christian
author_facet Kim, June-Young
Won, Ho-Yeon
Weiss, Christian
contents The flavor-nonsinglet ($u - d$) quark angular momentum (AM) in the proton is computed based on the effective spin-flavor dynamics emerging from chiral symmetry breaking by QCD instantons. The QCD AM operators are converted to effective spin-flavor operators expressing instanton-induced chiral interactions. A large negative orbital AM $L_{u - d}$ arises as a ``chiral magnetic effect'' of the interaction of the quarks with the chiral mean field in the proton in the large-$N_c$ limit. It cancels part of the large positive spin AM $S_{u-d}$ and reduces the total AM $J_{u-d} = L_{u-d} + S_{u-d}$, in agreement with lattice QCD calculations.
format Preprint
id arxiv_https___arxiv_org_abs_2605_23125
institution arXiv
publishDate 2026
record_format arxiv
spellingShingle Quark orbital angular momentum as a chiral magnetic effect
Kim, June-Young
Won, Ho-Yeon
Weiss, Christian
High Energy Physics - Phenomenology
The flavor-nonsinglet ($u - d$) quark angular momentum (AM) in the proton is computed based on the effective spin-flavor dynamics emerging from chiral symmetry breaking by QCD instantons. The QCD AM operators are converted to effective spin-flavor operators expressing instanton-induced chiral interactions. A large negative orbital AM $L_{u - d}$ arises as a ``chiral magnetic effect'' of the interaction of the quarks with the chiral mean field in the proton in the large-$N_c$ limit. It cancels part of the large positive spin AM $S_{u-d}$ and reduces the total AM $J_{u-d} = L_{u-d} + S_{u-d}$, in agreement with lattice QCD calculations.
title Quark orbital angular momentum as a chiral magnetic effect
topic High Energy Physics - Phenomenology
url https://arxiv.org/abs/2605.23125