Peer-reviewedCC BYPhysics Letters B
Quark orbital angular momentum from chiral symmetry breaking in QCD
Abstract
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 from the interactions 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.
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BibTeX
@article{kim2026quark,
title = {{Quark orbital angular momentum from chiral symmetry breaking in QCD}},
author = {June-Young Kim and Ho-Yeon Won and Christian Weiss},
journal = {Physics Letters B},
year = {2026},
month = sep,
doi = {10.1016/j.physletb.2026.140980},
url = {https://hal.science/hal-05767307v1},
note = {CC BY},
}
RIS
TY - JOUR
TI - Quark orbital angular momentum from chiral symmetry breaking in QCD
AU - June-Young Kim
AU - Ho-Yeon Won
AU - Christian Weiss
PY - 2026
DA - 2026/09/28
JO - Physics Letters B
DO - 10.1016/j.physletb.2026.140980
UR - https://hal.science/hal-05767307v1
AB - 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 from the interactions 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.
SN - 0370-2693
SN - 1873-2445
ER -