{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:2HMEKI6KNG6KS2MDL5BFERO27C","short_pith_number":"pith:2HMEKI6K","schema_version":"1.0","canonical_sha256":"d1d84523ca69bca969835f425245daf89edb48278a74655837677002250f8ebd","source":{"kind":"arxiv","id":"hep-ph/0212105","version":2},"attestation_state":"computed","paper":{"title":"Relating a gluon mass scale to an infrared fixed point in pure gauge QCD","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"A.A.Natale, A.C.Aguilar, P.S.Rodrigues da Silva (IFT-Unesp, Sao Paulo)","submitted_at":"2002-12-06T17:41:23Z","abstract_excerpt":"We show that in pure gauge QCD (or any pure non-Abelian gauge theory) the condition for the existence of a global minimum of energy with a gluon (gauge boson) mass scale also implies the existence of a fixed point of the $\\beta$ function. We argue that the frozen value of the coupling constant found in some solutions of the Schwinger-Dyson equations of QCD can be related to this fixed point. We also discuss how the inclusion of fermions modifies this property."},"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/0212105","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2002-12-06T17:41:23Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"60bd33bb1c3d8581b297aec5a297e7643003308783ce0ab5b9cbecbfe9ea1810","abstract_canon_sha256":"c31df0abc71a04b86f00bc35fe56c54da01b7ffaf6f0f75ae7f2c38ffb266b4b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:34:29.344281Z","signature_b64":"lcRx42v+Drbm9mNKT6Y+ElOgYhtr2aTeLa3eIisrWJJ6FJ/BlDqS2LCtfyG7RlKduwu/sRcX0k/ryWT7xpCtCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d1d84523ca69bca969835f425245daf89edb48278a74655837677002250f8ebd","last_reissued_at":"2026-07-04T16:34:29.343944Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:34:29.343944Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Relating a gluon mass scale to an infrared fixed point in pure gauge QCD","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"A.A.Natale, A.C.Aguilar, P.S.Rodrigues da Silva (IFT-Unesp, Sao Paulo)","submitted_at":"2002-12-06T17:41:23Z","abstract_excerpt":"We show that in pure gauge QCD (or any pure non-Abelian gauge theory) the condition for the existence of a global minimum of energy with a gluon (gauge boson) mass scale also implies the existence of a fixed point of the $\\beta$ function. We argue that the frozen value of the coupling constant found in some solutions of the Schwinger-Dyson equations of QCD can be related to this fixed point. We also discuss how the inclusion of fermions modifies this property."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0212105","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/0212105/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/0212105","created_at":"2026-07-04T16:34:29.343999+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0212105v2","created_at":"2026-07-04T16:34:29.343999+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0212105","created_at":"2026-07-04T16:34:29.343999+00:00"},{"alias_kind":"pith_short_12","alias_value":"2HMEKI6KNG6K","created_at":"2026-07-04T16:34:29.343999+00:00"},{"alias_kind":"pith_short_16","alias_value":"2HMEKI6KNG6KS2MD","created_at":"2026-07-04T16:34:29.343999+00:00"},{"alias_kind":"pith_short_8","alias_value":"2HMEKI6K","created_at":"2026-07-04T16:34:29.343999+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2HMEKI6KNG6KS2MDL5BFERO27C","json":"https://pith.science/pith/2HMEKI6KNG6KS2MDL5BFERO27C.json","graph_json":"https://pith.science/api/pith-number/2HMEKI6KNG6KS2MDL5BFERO27C/graph.json","events_json":"https://pith.science/api/pith-number/2HMEKI6KNG6KS2MDL5BFERO27C/events.json","paper":"https://pith.science/paper/2HMEKI6K"},"agent_actions":{"view_html":"https://pith.science/pith/2HMEKI6KNG6KS2MDL5BFERO27C","download_json":"https://pith.science/pith/2HMEKI6KNG6KS2MDL5BFERO27C.json","view_paper":"https://pith.science/paper/2HMEKI6K","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0212105&json=true","fetch_graph":"https://pith.science/api/pith-number/2HMEKI6KNG6KS2MDL5BFERO27C/graph.json","fetch_events":"https://pith.science/api/pith-number/2HMEKI6KNG6KS2MDL5BFERO27C/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2HMEKI6KNG6KS2MDL5BFERO27C/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2HMEKI6KNG6KS2MDL5BFERO27C/action/storage_attestation","attest_author":"https://pith.science/pith/2HMEKI6KNG6KS2MDL5BFERO27C/action/author_attestation","sign_citation":"https://pith.science/pith/2HMEKI6KNG6KS2MDL5BFERO27C/action/citation_signature","submit_replication":"https://pith.science/pith/2HMEKI6KNG6KS2MDL5BFERO27C/action/replication_record"}},"created_at":"2026-07-04T16:34:29.343999+00:00","updated_at":"2026-07-04T16:34:29.343999+00:00"}