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The quark propagators are computed on domain wall fermion configurations generated by the RBC-UKQCD Collaborations with $N_f=2+1$ flavors. Three ensembles with different light sea quark masses are used at one lattice spacing $1/a=1.75(4)$ GeV. We obtain $\\langle\\bar\\psi\\psi\\rangle^{\\overline{\\rm MS}}(2\\mbox{ GeV})=(-305(15)(21)\\mbox{ MeV})^3$ in the SU(2) chiral limit."},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1612.04579","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2016-12-14T11:18:15Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"f11423357ba9ffbfb098b3ebf774aa906942f5ed7047d76a3d616ee8da17d530","abstract_canon_sha256":"acc13ea64d2d9668f0de68249d637d9e336240a2cfe6f789afe6ab7caae7d327"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:32:14.247090Z","signature_b64":"g/ViONUziYnJo7/xTf69RaI/39qBnL+QqQftVBDHciMenvsVvJcQEoS7MF1LBBlzkcIiAkufq0t1m3EQ+lqvCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ec0e1742bb3c021093acebeb1e673a130fa86b0bebf419b01965dadaa64e8f39","last_reissued_at":"2026-05-18T00:32:14.246478Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:32:14.246478Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quark chiral condensate from the overlap quark propagator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Chao Wang, Hao Cai, Ming Gong, Ying Chen, Yujiang Bi, Zhaofeng Liu","submitted_at":"2016-12-14T11:18:15Z","abstract_excerpt":"From the overlap lattice quark propagator calculated in the Landau gauge, we determine the quark chiral condensate by fitting operator product expansion formulas to the lattice data. 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