{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:RHZ4A7ILQNCQRW3C2PJAQF4A5W","short_pith_number":"pith:RHZ4A7IL","schema_version":"1.0","canonical_sha256":"89f3c07d0b834508db62d3d2081780ed9af3144540f6f2e141be57429a28d253","source":{"kind":"arxiv","id":"1610.09708","version":1},"attestation_state":"computed","paper":{"title":"Complete Monopole Dominance of the Static Quark Potential","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Nigel Cundy","submitted_at":"2016-10-30T20:39:04Z","abstract_excerpt":"In earlier work, we used a gauge independent Abelian Decomposition to show that Abelian degrees of freedom are wholly responsible for the static quark potential. The restricted Abelian field can be split into two terms, a Maxwell term and a $\\theta$ (Dirac) term. The $\\theta$ term's contribution to the string tension can be analysed theoretically and numerically, and arises because of the existence of a certain type of monopole. While the Abelian field can be constructed without gauge fixing, its two component parts are gauge-dependent, with a gauge transformation moving the topological featur"},"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":"1610.09708","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2016-10-30T20:39:04Z","cross_cats_sorted":[],"title_canon_sha256":"9e80731796822ac7ae74ec5698cbe69a9a4cd3cb3036a8c31ead8cd29740c628","abstract_canon_sha256":"a80894e369276c279abcadbff28ff28b262ed97467d4a15b598c079700ca0001"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:00:51.259472Z","signature_b64":"zdjbLGISzub6Ht8/tM416/rIFS713QbR2xHmD7v7crjCg8zNcY/Can0Jsow6Np3DN8cG8MeD8A9LB340SKGzAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"89f3c07d0b834508db62d3d2081780ed9af3144540f6f2e141be57429a28d253","last_reissued_at":"2026-05-18T01:00:51.258846Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:00:51.258846Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Complete Monopole Dominance of the Static Quark Potential","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Nigel Cundy","submitted_at":"2016-10-30T20:39:04Z","abstract_excerpt":"In earlier work, we used a gauge independent Abelian Decomposition to show that Abelian degrees of freedom are wholly responsible for the static quark potential. The restricted Abelian field can be split into two terms, a Maxwell term and a $\\theta$ (Dirac) term. The $\\theta$ term's contribution to the string tension can be analysed theoretically and numerically, and arises because of the existence of a certain type of monopole. While the Abelian field can be constructed without gauge fixing, its two component parts are gauge-dependent, with a gauge transformation moving the topological featur"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.09708","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":"1610.09708","created_at":"2026-05-18T01:00:51.258943+00:00"},{"alias_kind":"arxiv_version","alias_value":"1610.09708v1","created_at":"2026-05-18T01:00:51.258943+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.09708","created_at":"2026-05-18T01:00:51.258943+00:00"},{"alias_kind":"pith_short_12","alias_value":"RHZ4A7ILQNCQ","created_at":"2026-05-18T12:30:41.710351+00:00"},{"alias_kind":"pith_short_16","alias_value":"RHZ4A7ILQNCQRW3C","created_at":"2026-05-18T12:30:41.710351+00:00"},{"alias_kind":"pith_short_8","alias_value":"RHZ4A7IL","created_at":"2026-05-18T12:30:41.710351+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/RHZ4A7ILQNCQRW3C2PJAQF4A5W","json":"https://pith.science/pith/RHZ4A7ILQNCQRW3C2PJAQF4A5W.json","graph_json":"https://pith.science/api/pith-number/RHZ4A7ILQNCQRW3C2PJAQF4A5W/graph.json","events_json":"https://pith.science/api/pith-number/RHZ4A7ILQNCQRW3C2PJAQF4A5W/events.json","paper":"https://pith.science/paper/RHZ4A7IL"},"agent_actions":{"view_html":"https://pith.science/pith/RHZ4A7ILQNCQRW3C2PJAQF4A5W","download_json":"https://pith.science/pith/RHZ4A7ILQNCQRW3C2PJAQF4A5W.json","view_paper":"https://pith.science/paper/RHZ4A7IL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1610.09708&json=true","fetch_graph":"https://pith.science/api/pith-number/RHZ4A7ILQNCQRW3C2PJAQF4A5W/graph.json","fetch_events":"https://pith.science/api/pith-number/RHZ4A7ILQNCQRW3C2PJAQF4A5W/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RHZ4A7ILQNCQRW3C2PJAQF4A5W/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RHZ4A7ILQNCQRW3C2PJAQF4A5W/action/storage_attestation","attest_author":"https://pith.science/pith/RHZ4A7ILQNCQRW3C2PJAQF4A5W/action/author_attestation","sign_citation":"https://pith.science/pith/RHZ4A7ILQNCQRW3C2PJAQF4A5W/action/citation_signature","submit_replication":"https://pith.science/pith/RHZ4A7ILQNCQRW3C2PJAQF4A5W/action/replication_record"}},"created_at":"2026-05-18T01:00:51.258943+00:00","updated_at":"2026-05-18T01:00:51.258943+00:00"}