{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1995:PQUFYI3TLAKOFDBNIZ2LBUMCSU","short_pith_number":"pith:PQUFYI3T","schema_version":"1.0","canonical_sha256":"7c285c23735814e28c2d4674b0d18295294a785fe3fb5211326fdd4ad5cc8891","source":{"kind":"arxiv","id":"hep-lat/9509039","version":1},"attestation_state":"computed","paper":{"title":"Critical Behavior of the Schwinger Model with Wilson Fermions","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A.F. Grillo, A. Galante, G. Di Carlo, V. Azcoiti, V. Laliena","submitted_at":"1995-09-13T13:23:32Z","abstract_excerpt":"We present a detailed analysis, in the framework of the MFA approach, of the critical behaviour of the lattice Schwinger model with Wilson fermions on lattices up to $24^2$, through the study of the Lee-Yang zeros and the specific heat. We find compelling evidence for a critical line ending at $\\kappa = 0.25$ at large $\\beta$. Finite size scaling analysis on lattices $8^2,12^2,16^2, 20^2$ and $24^2$ indicates a continuous transition. The hyperscaling relation is verified in the explored $\\beta$ region."},"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/9509039","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1995-09-13T13:23:32Z","cross_cats_sorted":[],"title_canon_sha256":"db99af94e5646029d705f0fd862c0514c06ab467659f31c3402a693f18a03666","abstract_canon_sha256":"b687495d9aefed08f51838b2a9867a6486ac19b7809d1448f28b37187d9025ce"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:58:55.753434Z","signature_b64":"eeylIA4zJ0Sfu1xCPv9PFBe8SaQccjS6nnlXN7eyGAvBHduv/CuJehnOhwea5V2WpzX/2fGjBudQ3frHagdSAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7c285c23735814e28c2d4674b0d18295294a785fe3fb5211326fdd4ad5cc8891","last_reissued_at":"2026-07-04T15:58:55.753000Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:58:55.753000Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Critical Behavior of the Schwinger Model with Wilson Fermions","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A.F. Grillo, A. Galante, G. Di Carlo, V. Azcoiti, V. Laliena","submitted_at":"1995-09-13T13:23:32Z","abstract_excerpt":"We present a detailed analysis, in the framework of the MFA approach, of the critical behaviour of the lattice Schwinger model with Wilson fermions on lattices up to $24^2$, through the study of the Lee-Yang zeros and the specific heat. We find compelling evidence for a critical line ending at $\\kappa = 0.25$ at large $\\beta$. Finite size scaling analysis on lattices $8^2,12^2,16^2, 20^2$ and $24^2$ indicates a continuous transition. The hyperscaling relation is verified in the explored $\\beta$ region."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9509039","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/9509039/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/9509039","created_at":"2026-07-04T15:58:55.753073+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9509039v1","created_at":"2026-07-04T15:58:55.753073+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9509039","created_at":"2026-07-04T15:58:55.753073+00:00"},{"alias_kind":"pith_short_12","alias_value":"PQUFYI3TLAKO","created_at":"2026-07-04T15:58:55.753073+00:00"},{"alias_kind":"pith_short_16","alias_value":"PQUFYI3TLAKOFDBN","created_at":"2026-07-04T15:58:55.753073+00:00"},{"alias_kind":"pith_short_8","alias_value":"PQUFYI3T","created_at":"2026-07-04T15:58:55.753073+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/PQUFYI3TLAKOFDBNIZ2LBUMCSU","json":"https://pith.science/pith/PQUFYI3TLAKOFDBNIZ2LBUMCSU.json","graph_json":"https://pith.science/api/pith-number/PQUFYI3TLAKOFDBNIZ2LBUMCSU/graph.json","events_json":"https://pith.science/api/pith-number/PQUFYI3TLAKOFDBNIZ2LBUMCSU/events.json","paper":"https://pith.science/paper/PQUFYI3T"},"agent_actions":{"view_html":"https://pith.science/pith/PQUFYI3TLAKOFDBNIZ2LBUMCSU","download_json":"https://pith.science/pith/PQUFYI3TLAKOFDBNIZ2LBUMCSU.json","view_paper":"https://pith.science/paper/PQUFYI3T","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/9509039&json=true","fetch_graph":"https://pith.science/api/pith-number/PQUFYI3TLAKOFDBNIZ2LBUMCSU/graph.json","fetch_events":"https://pith.science/api/pith-number/PQUFYI3TLAKOFDBNIZ2LBUMCSU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PQUFYI3TLAKOFDBNIZ2LBUMCSU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PQUFYI3TLAKOFDBNIZ2LBUMCSU/action/storage_attestation","attest_author":"https://pith.science/pith/PQUFYI3TLAKOFDBNIZ2LBUMCSU/action/author_attestation","sign_citation":"https://pith.science/pith/PQUFYI3TLAKOFDBNIZ2LBUMCSU/action/citation_signature","submit_replication":"https://pith.science/pith/PQUFYI3TLAKOFDBNIZ2LBUMCSU/action/replication_record"}},"created_at":"2026-07-04T15:58:55.753073+00:00","updated_at":"2026-07-04T15:58:55.753073+00:00"}