{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2000:APHM5O4HETASTQOOCD5CKJK4FC","short_pith_number":"pith:APHM5O4H","schema_version":"1.0","canonical_sha256":"03cecebb8724c129c1ce10fa25255c2890144b384f75a3b6b852601254bc5425","source":{"kind":"arxiv","id":"hep-th/0004158","version":3},"attestation_state":"computed","paper":{"title":"Abelian dominance in low-energy Gluodynamics due to dynamical mass generation","license":"","headline":"","cross_cats":["hep-lat","hep-ph"],"primary_cat":"hep-th","authors_text":"K.-I. Kondo, T. Shinohara (Chiba Univ.)","submitted_at":"2000-04-24T07:12:45Z","abstract_excerpt":"We show that off-diagonal gluons and off-diagonal ghosts acquire their masses dynamically in QCD if the maximal Abelian gauge is adopted. This result strongly supports the Abelian dominance in low-energy region of QCD. The mass generation is shown to occur due to ghost-anti-ghost condensation caused by attractive quartic ghost interactions within the Abelian projected effective gauge theory (derived by one of the authors). In fact, the quartic ghost interaction is indispensable for the renormalizability due to nonlinearity of the maximal Abelian gauge. The ghost-anti-ghost condensation is asso"},"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-th/0004158","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2000-04-24T07:12:45Z","cross_cats_sorted":["hep-lat","hep-ph"],"title_canon_sha256":"e9935e4c704b3e3b9ff3f652face99d82d84e62031818eb3b4edb12a52daea22","abstract_canon_sha256":"1c4ce4b4de392e1859a1e636bbdaa2f969e5c288a617e6958418815bc26cefbf"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:20:44.746469Z","signature_b64":"klWjhSuok8s2qxKWKdn13bIZENQg4nCefoCFZTmSMUuOtKySAiWCFiiI5hLGS163mQ+SSl49mk2Jucnd7i0ZAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"03cecebb8724c129c1ce10fa25255c2890144b384f75a3b6b852601254bc5425","last_reissued_at":"2026-07-04T16:20:44.746035Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:20:44.746035Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Abelian dominance in low-energy Gluodynamics due to dynamical mass generation","license":"","headline":"","cross_cats":["hep-lat","hep-ph"],"primary_cat":"hep-th","authors_text":"K.-I. Kondo, T. Shinohara (Chiba Univ.)","submitted_at":"2000-04-24T07:12:45Z","abstract_excerpt":"We show that off-diagonal gluons and off-diagonal ghosts acquire their masses dynamically in QCD if the maximal Abelian gauge is adopted. This result strongly supports the Abelian dominance in low-energy region of QCD. The mass generation is shown to occur due to ghost-anti-ghost condensation caused by attractive quartic ghost interactions within the Abelian projected effective gauge theory (derived by one of the authors). In fact, the quartic ghost interaction is indispensable for the renormalizability due to nonlinearity of the maximal Abelian gauge. The ghost-anti-ghost condensation is asso"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0004158","kind":"arxiv","version":3},"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-th/0004158/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-th/0004158","created_at":"2026-07-04T16:20:44.746096+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0004158v3","created_at":"2026-07-04T16:20:44.746096+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0004158","created_at":"2026-07-04T16:20:44.746096+00:00"},{"alias_kind":"pith_short_12","alias_value":"APHM5O4HETAS","created_at":"2026-07-04T16:20:44.746096+00:00"},{"alias_kind":"pith_short_16","alias_value":"APHM5O4HETASTQOO","created_at":"2026-07-04T16:20:44.746096+00:00"},{"alias_kind":"pith_short_8","alias_value":"APHM5O4H","created_at":"2026-07-04T16:20:44.746096+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1908.08753","citing_title":"Perturbative static quark potential in Maximal Abelian gauge","ref_index":274,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/APHM5O4HETASTQOOCD5CKJK4FC","json":"https://pith.science/pith/APHM5O4HETASTQOOCD5CKJK4FC.json","graph_json":"https://pith.science/api/pith-number/APHM5O4HETASTQOOCD5CKJK4FC/graph.json","events_json":"https://pith.science/api/pith-number/APHM5O4HETASTQOOCD5CKJK4FC/events.json","paper":"https://pith.science/paper/APHM5O4H"},"agent_actions":{"view_html":"https://pith.science/pith/APHM5O4HETASTQOOCD5CKJK4FC","download_json":"https://pith.science/pith/APHM5O4HETASTQOOCD5CKJK4FC.json","view_paper":"https://pith.science/paper/APHM5O4H","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0004158&json=true","fetch_graph":"https://pith.science/api/pith-number/APHM5O4HETASTQOOCD5CKJK4FC/graph.json","fetch_events":"https://pith.science/api/pith-number/APHM5O4HETASTQOOCD5CKJK4FC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/APHM5O4HETASTQOOCD5CKJK4FC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/APHM5O4HETASTQOOCD5CKJK4FC/action/storage_attestation","attest_author":"https://pith.science/pith/APHM5O4HETASTQOOCD5CKJK4FC/action/author_attestation","sign_citation":"https://pith.science/pith/APHM5O4HETASTQOOCD5CKJK4FC/action/citation_signature","submit_replication":"https://pith.science/pith/APHM5O4HETASTQOOCD5CKJK4FC/action/replication_record"}},"created_at":"2026-07-04T16:20:44.746096+00:00","updated_at":"2026-07-04T16:20:44.746096+00:00"}