{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:V7YTNXB3V25CN32HQL6YYA2MD2","short_pith_number":"pith:V7YTNXB3","schema_version":"1.0","canonical_sha256":"aff136dc3baeba26ef4782fd8c034c1e87c874dea6076f261463e6c5cffd7186","source":{"kind":"arxiv","id":"hep-lat/9805007","version":1},"attestation_state":"computed","paper":{"title":"Lattice Chiral Schwinger Model: Selected Results","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Thimm, G. Schierholz, V. Bornyakov","submitted_at":"1998-05-08T16:14:42Z","abstract_excerpt":"We discuss a method for regularizing chiral gauge theories. The idea is to formulate the gauge fields on the lattice, while the fermion determinant is regularized and computed in the continuum. A simple effective action emerges which lends itself to numerical simulations."},"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-lat/9805007","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1998-05-08T16:14:42Z","cross_cats_sorted":[],"title_canon_sha256":"e8416fde73ab6768a6f72ffce6b877808d1e41d7790b3d0458483efca137a5f3","abstract_canon_sha256":"c1ba2635976d17d36ce547dcbf12d0efeedf39760bd554ea4fa682e3dd71eb2f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:27:18.262533Z","signature_b64":"5ESDJEXJwdvSSK+SamZ4wP+EyYxyJBcC20tOdbvXuEMDcFS56/HeoFWW/noO5O+KJ38vSfvhFih4q67QZrxNBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aff136dc3baeba26ef4782fd8c034c1e87c874dea6076f261463e6c5cffd7186","last_reissued_at":"2026-07-04T14:27:18.262170Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:27:18.262170Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Lattice Chiral Schwinger Model: Selected Results","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Thimm, G. Schierholz, V. Bornyakov","submitted_at":"1998-05-08T16:14:42Z","abstract_excerpt":"We discuss a method for regularizing chiral gauge theories. The idea is to formulate the gauge fields on the lattice, while the fermion determinant is regularized and computed in the continuum. A simple effective action emerges which lends itself to numerical simulations."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9805007","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-lat/9805007/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":"hep-lat/9805007","created_at":"2026-07-04T14:27:18.262225+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9805007v1","created_at":"2026-07-04T14:27:18.262225+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9805007","created_at":"2026-07-04T14:27:18.262225+00:00"},{"alias_kind":"pith_short_12","alias_value":"V7YTNXB3V25C","created_at":"2026-07-04T14:27:18.262225+00:00"},{"alias_kind":"pith_short_16","alias_value":"V7YTNXB3V25CN32H","created_at":"2026-07-04T14:27:18.262225+00:00"},{"alias_kind":"pith_short_8","alias_value":"V7YTNXB3","created_at":"2026-07-04T14:27:18.262225+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/V7YTNXB3V25CN32HQL6YYA2MD2","json":"https://pith.science/pith/V7YTNXB3V25CN32HQL6YYA2MD2.json","graph_json":"https://pith.science/api/pith-number/V7YTNXB3V25CN32HQL6YYA2MD2/graph.json","events_json":"https://pith.science/api/pith-number/V7YTNXB3V25CN32HQL6YYA2MD2/events.json","paper":"https://pith.science/paper/V7YTNXB3"},"agent_actions":{"view_html":"https://pith.science/pith/V7YTNXB3V25CN32HQL6YYA2MD2","download_json":"https://pith.science/pith/V7YTNXB3V25CN32HQL6YYA2MD2.json","view_paper":"https://pith.science/paper/V7YTNXB3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/9805007&json=true","fetch_graph":"https://pith.science/api/pith-number/V7YTNXB3V25CN32HQL6YYA2MD2/graph.json","fetch_events":"https://pith.science/api/pith-number/V7YTNXB3V25CN32HQL6YYA2MD2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/V7YTNXB3V25CN32HQL6YYA2MD2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/V7YTNXB3V25CN32HQL6YYA2MD2/action/storage_attestation","attest_author":"https://pith.science/pith/V7YTNXB3V25CN32HQL6YYA2MD2/action/author_attestation","sign_citation":"https://pith.science/pith/V7YTNXB3V25CN32HQL6YYA2MD2/action/citation_signature","submit_replication":"https://pith.science/pith/V7YTNXB3V25CN32HQL6YYA2MD2/action/replication_record"}},"created_at":"2026-07-04T14:27:18.262225+00:00","updated_at":"2026-07-04T14:27:18.262225+00:00"}