{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:6EGBLFJH7IRARCBDJT6SFAPS3B","short_pith_number":"pith:6EGBLFJH","schema_version":"1.0","canonical_sha256":"f10c159527fa220888234cfd2281f2d868e0b372961ca8f58440a22dee4e7db1","source":{"kind":"arxiv","id":"2110.10573","version":2},"attestation_state":"computed","paper":{"title":"Proca Theory from the Spinning Worldline","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Ivo Sachs, Matthias Carosi","submitted_at":"2021-10-20T14:02:57Z","abstract_excerpt":"We obtain Proca field theory from the quantisation of the $\\mathcal{N}=2$ supersymmetric worldline upon supplementing the graded BRST-algebra with an extra multiplet of oscillators. The linearised theory describes the BV-extended spectrum of Proca theory, together with a St\\\"uckelberg field. When coupling the theory to background fields we derive the Proca equations, arising as consistency conditions in the BRST procedure. We also explore non-abelian modifications, complexified vector fields as well as coupling to a dilaton field. We propose a cubic action on the space of BRST-operators which "},"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":"2110.10573","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2021-10-20T14:02:57Z","cross_cats_sorted":[],"title_canon_sha256":"d72c5a137487f44a076db52444d5b829c42ad2a3f5aeceb2a2541bd990e588b4","abstract_canon_sha256":"790cd62a6367188c5a30b031baa74a9b31bb2fa313e185236ca18592ccb7c8fb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:51:45.126168Z","signature_b64":"bIG0rCKVPLiO44QavfCeONswMsiZ4mliAXJIXUazKvUtaSol4AElO2wQIDGneTmmyQWsesn1kjDCGbzZELD+AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f10c159527fa220888234cfd2281f2d868e0b372961ca8f58440a22dee4e7db1","last_reissued_at":"2026-07-05T03:51:45.125714Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:51:45.125714Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Proca Theory from the Spinning Worldline","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Ivo Sachs, Matthias Carosi","submitted_at":"2021-10-20T14:02:57Z","abstract_excerpt":"We obtain Proca field theory from the quantisation of the $\\mathcal{N}=2$ supersymmetric worldline upon supplementing the graded BRST-algebra with an extra multiplet of oscillators. The linearised theory describes the BV-extended spectrum of Proca theory, together with a St\\\"uckelberg field. When coupling the theory to background fields we derive the Proca equations, arising as consistency conditions in the BRST procedure. We also explore non-abelian modifications, complexified vector fields as well as coupling to a dilaton field. We propose a cubic action on the space of BRST-operators which "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2110.10573","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/2110.10573/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":"2110.10573","created_at":"2026-07-05T03:51:45.125774+00:00"},{"alias_kind":"arxiv_version","alias_value":"2110.10573v2","created_at":"2026-07-05T03:51:45.125774+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2110.10573","created_at":"2026-07-05T03:51:45.125774+00:00"},{"alias_kind":"pith_short_12","alias_value":"6EGBLFJH7IRA","created_at":"2026-07-05T03:51:45.125774+00:00"},{"alias_kind":"pith_short_16","alias_value":"6EGBLFJH7IRARCBD","created_at":"2026-07-05T03:51:45.125774+00:00"},{"alias_kind":"pith_short_8","alias_value":"6EGBLFJH","created_at":"2026-07-05T03:51:45.125774+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.15943","citing_title":"Pair production of massive charged vector bosons from the worldline","ref_index":2022,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6EGBLFJH7IRARCBDJT6SFAPS3B","json":"https://pith.science/pith/6EGBLFJH7IRARCBDJT6SFAPS3B.json","graph_json":"https://pith.science/api/pith-number/6EGBLFJH7IRARCBDJT6SFAPS3B/graph.json","events_json":"https://pith.science/api/pith-number/6EGBLFJH7IRARCBDJT6SFAPS3B/events.json","paper":"https://pith.science/paper/6EGBLFJH"},"agent_actions":{"view_html":"https://pith.science/pith/6EGBLFJH7IRARCBDJT6SFAPS3B","download_json":"https://pith.science/pith/6EGBLFJH7IRARCBDJT6SFAPS3B.json","view_paper":"https://pith.science/paper/6EGBLFJH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2110.10573&json=true","fetch_graph":"https://pith.science/api/pith-number/6EGBLFJH7IRARCBDJT6SFAPS3B/graph.json","fetch_events":"https://pith.science/api/pith-number/6EGBLFJH7IRARCBDJT6SFAPS3B/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6EGBLFJH7IRARCBDJT6SFAPS3B/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6EGBLFJH7IRARCBDJT6SFAPS3B/action/storage_attestation","attest_author":"https://pith.science/pith/6EGBLFJH7IRARCBDJT6SFAPS3B/action/author_attestation","sign_citation":"https://pith.science/pith/6EGBLFJH7IRARCBDJT6SFAPS3B/action/citation_signature","submit_replication":"https://pith.science/pith/6EGBLFJH7IRARCBDJT6SFAPS3B/action/replication_record"}},"created_at":"2026-07-05T03:51:45.125774+00:00","updated_at":"2026-07-05T03:51:45.125774+00:00"}