{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:6HCVIJOWDQLHWBRUAPUUZSW47Z","short_pith_number":"pith:6HCVIJOW","schema_version":"1.0","canonical_sha256":"f1c55425d61c167b063403e94ccadcfe78bf764dfacbb9222ad389ba0f75964c","source":{"kind":"arxiv","id":"1604.00046","version":1},"attestation_state":"computed","paper":{"title":"Noncommutative geometry and the BV formalism: application to a matrix model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math.MP"],"primary_cat":"math-ph","authors_text":"Roberta A. Iseppi, Walter D. van Suijlekom","submitted_at":"2016-03-31T20:40:08Z","abstract_excerpt":"We analyze a U(2)-matrix model derived from a finite spectral triple. By applying the BV formalism, we find a general solution to the classical master equation. To describe the BV formalism in the context of noncommutative geometry, we define two finite spectral triples: the BV spectral triple and the BV auxiliary spectral triple. These are constructed from the gauge fields, ghost fields and anti-fields that enter the BV construction. We show that their fermionic actions add up precisely to the BV action. This approach allows for a geometric description of the ghost fields and their properties"},"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":"1604.00046","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2016-03-31T20:40:08Z","cross_cats_sorted":["math.MP"],"title_canon_sha256":"c845d179480e462d3e108a412b66c9bc6d38a1343a953611ddd4ec964993a50f","abstract_canon_sha256":"eb2aab582563fec787621095ac98377036b3ec2df5ef0d802c058f174ffb5e4e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:37:01.852168Z","signature_b64":"+w7uYJ5KC79Y9aki5W/bNW4lIC7Mzmokn6Q4BFFlk3heuJPTUBvFbbHBMy6bDdghZNxCpqbPSkxLD1/ZXZLCCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f1c55425d61c167b063403e94ccadcfe78bf764dfacbb9222ad389ba0f75964c","last_reissued_at":"2026-05-18T00:37:01.851572Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:37:01.851572Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Noncommutative geometry and the BV formalism: application to a matrix model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math.MP"],"primary_cat":"math-ph","authors_text":"Roberta A. Iseppi, Walter D. van Suijlekom","submitted_at":"2016-03-31T20:40:08Z","abstract_excerpt":"We analyze a U(2)-matrix model derived from a finite spectral triple. By applying the BV formalism, we find a general solution to the classical master equation. To describe the BV formalism in the context of noncommutative geometry, we define two finite spectral triples: the BV spectral triple and the BV auxiliary spectral triple. These are constructed from the gauge fields, ghost fields and anti-fields that enter the BV construction. We show that their fermionic actions add up precisely to the BV action. This approach allows for a geometric description of the ghost fields and their properties"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.00046","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":"1604.00046","created_at":"2026-05-18T00:37:01.851659+00:00"},{"alias_kind":"arxiv_version","alias_value":"1604.00046v1","created_at":"2026-05-18T00:37:01.851659+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.00046","created_at":"2026-05-18T00:37:01.851659+00:00"},{"alias_kind":"pith_short_12","alias_value":"6HCVIJOWDQLH","created_at":"2026-05-18T12:30:01.593930+00:00"},{"alias_kind":"pith_short_16","alias_value":"6HCVIJOWDQLHWBRU","created_at":"2026-05-18T12:30:01.593930+00:00"},{"alias_kind":"pith_short_8","alias_value":"6HCVIJOW","created_at":"2026-05-18T12:30:01.593930+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/6HCVIJOWDQLHWBRUAPUUZSW47Z","json":"https://pith.science/pith/6HCVIJOWDQLHWBRUAPUUZSW47Z.json","graph_json":"https://pith.science/api/pith-number/6HCVIJOWDQLHWBRUAPUUZSW47Z/graph.json","events_json":"https://pith.science/api/pith-number/6HCVIJOWDQLHWBRUAPUUZSW47Z/events.json","paper":"https://pith.science/paper/6HCVIJOW"},"agent_actions":{"view_html":"https://pith.science/pith/6HCVIJOWDQLHWBRUAPUUZSW47Z","download_json":"https://pith.science/pith/6HCVIJOWDQLHWBRUAPUUZSW47Z.json","view_paper":"https://pith.science/paper/6HCVIJOW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1604.00046&json=true","fetch_graph":"https://pith.science/api/pith-number/6HCVIJOWDQLHWBRUAPUUZSW47Z/graph.json","fetch_events":"https://pith.science/api/pith-number/6HCVIJOWDQLHWBRUAPUUZSW47Z/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6HCVIJOWDQLHWBRUAPUUZSW47Z/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6HCVIJOWDQLHWBRUAPUUZSW47Z/action/storage_attestation","attest_author":"https://pith.science/pith/6HCVIJOWDQLHWBRUAPUUZSW47Z/action/author_attestation","sign_citation":"https://pith.science/pith/6HCVIJOWDQLHWBRUAPUUZSW47Z/action/citation_signature","submit_replication":"https://pith.science/pith/6HCVIJOWDQLHWBRUAPUUZSW47Z/action/replication_record"}},"created_at":"2026-05-18T00:37:01.851659+00:00","updated_at":"2026-05-18T00:37:01.851659+00:00"}