{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:ISLYQELFSL6GBH73ODIIX775AT","short_pith_number":"pith:ISLYQELF","schema_version":"1.0","canonical_sha256":"449788116592fc609ffb70d08bfffd04f28030c67dbd90d927ec38fbd1e0ca2a","source":{"kind":"arxiv","id":"hep-th/9611002","version":1},"attestation_state":"computed","paper":{"title":"Algebraic Renormalization of Parity-Preserving QED_3 Coupled to Scalar Matter II: Broken Case","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"D. H. T. Franco, J. A. Helay\\\"el-Neto, O. M. Del Cima, O. Piguet","submitted_at":"1996-11-01T13:29:59Z","abstract_excerpt":"In this letter the algebraic renormalization method, which is independent of any kind of regularization scheme, is presented for the parity-preserving QED_3 coupled to scalar matter in the broken regime, where the scalar assumes a finite vacuum expectation value, $<\\vf> = v$. The model shows to be stable under radiative corrections and anomaly free."},"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/9611002","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1996-11-01T13:29:59Z","cross_cats_sorted":[],"title_canon_sha256":"44b16851ae2a12c9f0659aeb879f04f7205a381fe33c806564ee1ccfd9d7d832","abstract_canon_sha256":"4b15f886b19092d022cf50f09e64c9b5e237bda000a826f6cb14c81aa6cd6a0a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:05:56.632784Z","signature_b64":"AX3eUklGtwKNM0exB+M1uNXKmGnsilvuS3c0lG+YBY5nASfpRaHfrSMOp+GUIWag/QdJSaXzY2cO4SjbRwjmAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"449788116592fc609ffb70d08bfffd04f28030c67dbd90d927ec38fbd1e0ca2a","last_reissued_at":"2026-05-18T01:05:56.632359Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:05:56.632359Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Algebraic Renormalization of Parity-Preserving QED_3 Coupled to Scalar Matter II: Broken Case","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"D. H. T. Franco, J. A. Helay\\\"el-Neto, O. M. Del Cima, O. Piguet","submitted_at":"1996-11-01T13:29:59Z","abstract_excerpt":"In this letter the algebraic renormalization method, which is independent of any kind of regularization scheme, is presented for the parity-preserving QED_3 coupled to scalar matter in the broken regime, where the scalar assumes a finite vacuum expectation value, $<\\vf> = v$. The model shows to be stable under radiative corrections and anomaly free."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9611002","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":"hep-th/9611002","created_at":"2026-05-18T01:05:56.632425+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9611002v1","created_at":"2026-05-18T01:05:56.632425+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9611002","created_at":"2026-05-18T01:05:56.632425+00:00"},{"alias_kind":"pith_short_12","alias_value":"ISLYQELFSL6G","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_16","alias_value":"ISLYQELFSL6GBH73","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_8","alias_value":"ISLYQELF","created_at":"2026-05-18T12:25:47.700082+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/ISLYQELFSL6GBH73ODIIX775AT","json":"https://pith.science/pith/ISLYQELFSL6GBH73ODIIX775AT.json","graph_json":"https://pith.science/api/pith-number/ISLYQELFSL6GBH73ODIIX775AT/graph.json","events_json":"https://pith.science/api/pith-number/ISLYQELFSL6GBH73ODIIX775AT/events.json","paper":"https://pith.science/paper/ISLYQELF"},"agent_actions":{"view_html":"https://pith.science/pith/ISLYQELFSL6GBH73ODIIX775AT","download_json":"https://pith.science/pith/ISLYQELFSL6GBH73ODIIX775AT.json","view_paper":"https://pith.science/paper/ISLYQELF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9611002&json=true","fetch_graph":"https://pith.science/api/pith-number/ISLYQELFSL6GBH73ODIIX775AT/graph.json","fetch_events":"https://pith.science/api/pith-number/ISLYQELFSL6GBH73ODIIX775AT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ISLYQELFSL6GBH73ODIIX775AT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ISLYQELFSL6GBH73ODIIX775AT/action/storage_attestation","attest_author":"https://pith.science/pith/ISLYQELFSL6GBH73ODIIX775AT/action/author_attestation","sign_citation":"https://pith.science/pith/ISLYQELFSL6GBH73ODIIX775AT/action/citation_signature","submit_replication":"https://pith.science/pith/ISLYQELFSL6GBH73ODIIX775AT/action/replication_record"}},"created_at":"2026-05-18T01:05:56.632425+00:00","updated_at":"2026-05-18T01:05:56.632425+00:00"}