{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:DUJLZLGKLUMS3UWPN4MVHG6QKG","short_pith_number":"pith:DUJLZLGK","schema_version":"1.0","canonical_sha256":"1d12bcacca5d192dd2cf6f19539bd051bf56b45fe0f08843408e3de21fbbca8f","source":{"kind":"arxiv","id":"1603.03470","version":1},"attestation_state":"computed","paper":{"title":"Complete Monopole Dominance of the Yang-Mills Confining Potential","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-lat","authors_text":"Nigel Cundy, Weonjong Lee, Y. M. Cho","submitted_at":"2016-03-10T22:05:24Z","abstract_excerpt":"We continue our investigation of quark confinement using a particular variant of the Cho-Duan-Ge gauge independent Abelian decomposition. The decomposition splits the gauge field into a restricted Abelian part and a coloured part in a way that preserves gauge covariance. The restricted part of the gauge field can be divided into a Maxwell term and a topological term. Previously, we showed that by a particular choice of this decomposition we could fully describe the confining potential using only the restricted gauge field. We proposed that various topological objects (a form of magnetic monopo"},"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":"1603.03470","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2016-03-10T22:05:24Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"1f7f64db076ce7a6dd687e3a2556556e4b8efcad2ec68d85ebd70df273700c72","abstract_canon_sha256":"b27a804cf14cdec44776e8c290117984864e9f86d81494ce89035786e2c62d9e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:19:15.546719Z","signature_b64":"dZZ6WqPUktdiCOyklklNqCTBUwDiTSTSwJY429cJ32PBOE0OTVSIdgUd6GPPj+f8d/XkqkXZWNtzJrlmOkL6BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1d12bcacca5d192dd2cf6f19539bd051bf56b45fe0f08843408e3de21fbbca8f","last_reissued_at":"2026-05-18T01:19:15.546122Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:19:15.546122Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Complete Monopole Dominance of the Yang-Mills Confining Potential","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-lat","authors_text":"Nigel Cundy, Weonjong Lee, Y. M. Cho","submitted_at":"2016-03-10T22:05:24Z","abstract_excerpt":"We continue our investigation of quark confinement using a particular variant of the Cho-Duan-Ge gauge independent Abelian decomposition. The decomposition splits the gauge field into a restricted Abelian part and a coloured part in a way that preserves gauge covariance. The restricted part of the gauge field can be divided into a Maxwell term and a topological term. Previously, we showed that by a particular choice of this decomposition we could fully describe the confining potential using only the restricted gauge field. We proposed that various topological objects (a form of magnetic monopo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1603.03470","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"1603.03470","created_at":"2026-05-18T01:19:15.546201+00:00"},{"alias_kind":"arxiv_version","alias_value":"1603.03470v1","created_at":"2026-05-18T01:19:15.546201+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1603.03470","created_at":"2026-05-18T01:19:15.546201+00:00"},{"alias_kind":"pith_short_12","alias_value":"DUJLZLGKLUMS","created_at":"2026-05-18T12:30:12.583610+00:00"},{"alias_kind":"pith_short_16","alias_value":"DUJLZLGKLUMS3UWP","created_at":"2026-05-18T12:30:12.583610+00:00"},{"alias_kind":"pith_short_8","alias_value":"DUJLZLGK","created_at":"2026-05-18T12:30:12.583610+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/DUJLZLGKLUMS3UWPN4MVHG6QKG","json":"https://pith.science/pith/DUJLZLGKLUMS3UWPN4MVHG6QKG.json","graph_json":"https://pith.science/api/pith-number/DUJLZLGKLUMS3UWPN4MVHG6QKG/graph.json","events_json":"https://pith.science/api/pith-number/DUJLZLGKLUMS3UWPN4MVHG6QKG/events.json","paper":"https://pith.science/paper/DUJLZLGK"},"agent_actions":{"view_html":"https://pith.science/pith/DUJLZLGKLUMS3UWPN4MVHG6QKG","download_json":"https://pith.science/pith/DUJLZLGKLUMS3UWPN4MVHG6QKG.json","view_paper":"https://pith.science/paper/DUJLZLGK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1603.03470&json=true","fetch_graph":"https://pith.science/api/pith-number/DUJLZLGKLUMS3UWPN4MVHG6QKG/graph.json","fetch_events":"https://pith.science/api/pith-number/DUJLZLGKLUMS3UWPN4MVHG6QKG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DUJLZLGKLUMS3UWPN4MVHG6QKG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DUJLZLGKLUMS3UWPN4MVHG6QKG/action/storage_attestation","attest_author":"https://pith.science/pith/DUJLZLGKLUMS3UWPN4MVHG6QKG/action/author_attestation","sign_citation":"https://pith.science/pith/DUJLZLGKLUMS3UWPN4MVHG6QKG/action/citation_signature","submit_replication":"https://pith.science/pith/DUJLZLGKLUMS3UWPN4MVHG6QKG/action/replication_record"}},"created_at":"2026-05-18T01:19:15.546201+00:00","updated_at":"2026-05-18T01:19:15.546201+00:00"}