{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:J3OLLOZDK5XJAAI73PI33443IQ","short_pith_number":"pith:J3OLLOZD","schema_version":"1.0","canonical_sha256":"4edcb5bb23576e90011fdbd1bdf39b440dcc1f753216c23ec2e836608f21e1f6","source":{"kind":"arxiv","id":"hep-ph/0107141","version":2},"attestation_state":"computed","paper":{"title":"Gluon propagators and quark confinement","license":"","headline":"","cross_cats":["hep-lat","hep-th"],"primary_cat":"hep-ph","authors_text":"H. Reinhardt, J. Gattnar, K. Langfeld","submitted_at":"2001-07-12T19:11:24Z","abstract_excerpt":"The gluon propagator is investigated in Landau and in maximal center gauge for the gauge group SU(2) by means of lattice gauge simulations. We find that Gribov ambiguities arising from the implementation of Landau gauge have a small influence on the propagator. In agreement with previous findings, we obtain that the small momentum behavior is dominated by a mass, which is of order $(1.48 \\pm 0.05) \\sqrt{\\sigma}$, where $\\sigma $ is the string tension. By removing the confining vortices from the full Yang-Mills ensemble, we convert full YM-theory into a theory which does not confine quarks. We "},"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-ph/0107141","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-07-12T19:11:24Z","cross_cats_sorted":["hep-lat","hep-th"],"title_canon_sha256":"adb3f69aef863338829bd31cbffe2bad3a9189d7399430c0490c0451347ec450","abstract_canon_sha256":"6889564c1d0fe9f5be09846c16f36328aa00355525696ad0fcea6a9b0679dfca"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:27:24.874437Z","signature_b64":"NKNQNcOJ101yWxHCPDUJ8tICt4NJuLX+KwkC3yOeE+0h3IsX4EyIw1Y6gvT6sh4RKsrR3QkAqqUZL3+kB9A5BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4edcb5bb23576e90011fdbd1bdf39b440dcc1f753216c23ec2e836608f21e1f6","last_reissued_at":"2026-07-04T16:27:24.873997Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:27:24.873997Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gluon propagators and quark confinement","license":"","headline":"","cross_cats":["hep-lat","hep-th"],"primary_cat":"hep-ph","authors_text":"H. Reinhardt, J. Gattnar, K. Langfeld","submitted_at":"2001-07-12T19:11:24Z","abstract_excerpt":"The gluon propagator is investigated in Landau and in maximal center gauge for the gauge group SU(2) by means of lattice gauge simulations. We find that Gribov ambiguities arising from the implementation of Landau gauge have a small influence on the propagator. In agreement with previous findings, we obtain that the small momentum behavior is dominated by a mass, which is of order $(1.48 \\pm 0.05) \\sqrt{\\sigma}$, where $\\sigma $ is the string tension. By removing the confining vortices from the full Yang-Mills ensemble, we convert full YM-theory into a theory which does not confine quarks. We "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0107141","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/0107141/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0107141","created_at":"2026-07-04T16:27:24.874068+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0107141v2","created_at":"2026-07-04T16:27:24.874068+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0107141","created_at":"2026-07-04T16:27:24.874068+00:00"},{"alias_kind":"pith_short_12","alias_value":"J3OLLOZDK5XJ","created_at":"2026-07-04T16:27:24.874068+00:00"},{"alias_kind":"pith_short_16","alias_value":"J3OLLOZDK5XJAAI7","created_at":"2026-07-04T16:27:24.874068+00:00"},{"alias_kind":"pith_short_8","alias_value":"J3OLLOZD","created_at":"2026-07-04T16:27:24.874068+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.05807","citing_title":"Center vortices in the novel phase of staggered fermions","ref_index":28,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/J3OLLOZDK5XJAAI73PI33443IQ","json":"https://pith.science/pith/J3OLLOZDK5XJAAI73PI33443IQ.json","graph_json":"https://pith.science/api/pith-number/J3OLLOZDK5XJAAI73PI33443IQ/graph.json","events_json":"https://pith.science/api/pith-number/J3OLLOZDK5XJAAI73PI33443IQ/events.json","paper":"https://pith.science/paper/J3OLLOZD"},"agent_actions":{"view_html":"https://pith.science/pith/J3OLLOZDK5XJAAI73PI33443IQ","download_json":"https://pith.science/pith/J3OLLOZDK5XJAAI73PI33443IQ.json","view_paper":"https://pith.science/paper/J3OLLOZD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0107141&json=true","fetch_graph":"https://pith.science/api/pith-number/J3OLLOZDK5XJAAI73PI33443IQ/graph.json","fetch_events":"https://pith.science/api/pith-number/J3OLLOZDK5XJAAI73PI33443IQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/J3OLLOZDK5XJAAI73PI33443IQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/J3OLLOZDK5XJAAI73PI33443IQ/action/storage_attestation","attest_author":"https://pith.science/pith/J3OLLOZDK5XJAAI73PI33443IQ/action/author_attestation","sign_citation":"https://pith.science/pith/J3OLLOZDK5XJAAI73PI33443IQ/action/citation_signature","submit_replication":"https://pith.science/pith/J3OLLOZDK5XJAAI73PI33443IQ/action/replication_record"}},"created_at":"2026-07-04T16:27:24.874068+00:00","updated_at":"2026-07-04T16:27:24.874068+00:00"}