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We generate 100 gauge configurations on the 16^4 lattice with \\beta = 6.0, and measure the mixed condensate at 16 points in each gauge configuration for each current-quark mass of m_q=21, 36, 52 MeV. From the 1600 data for each m_q, we find the ratio between the mixed condensate and the quark condensate, m_0^2 = g<\\bar{q} sigma G q> / <\\bar{q}q> \\simeq 2.5 GeV^2 at the lattice scale of 1/a \\simeq 2 GeV i"},"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":"hep-lat/0212025","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2002-12-16T10:03:01Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"f58be5b4a8e9bbd192bddf1567db995b7b0a4cd26f09c7bd1d0ead7c2c1935c0","abstract_canon_sha256":"3d1716a28d997c61d5ea865be34e69706f9f2ec3738a024046671bcabc9dc8d8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:37:29.946405Z","signature_b64":"goD6lSZi4P1FheQECBwiVIM+wDTZLItaSOaPwslEpV9bPkmTQaS5ptd6jIu9jxKOA28sJyEv8WjrWzTgwarYAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dfcd071e528d0686b56db7e1f64f7db3f34356d09dc0eaa300ff5e8156be53cb","last_reissued_at":"2026-05-18T00:37:29.945862Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:37:29.945862Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Lattice QCD study for the Quark-Gluon Mixed Condensate (anti-Q sigma G Q)","license":"","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"(2) Wako, Hideo Suganuma (1) ((1) Tokyo Inst. 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