{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1993:3XRBPGEKB5LMHKYGJUEKZPMRPR","short_pith_number":"pith:3XRBPGEK","schema_version":"1.0","canonical_sha256":"dde217988a0f56c3ab064d08acbd917c6e0f19ceaaaff4f79984dd298cadf825","source":{"kind":"arxiv","id":"hep-lat/9311029","version":1},"attestation_state":"computed","paper":{"title":"Scaling and Density of Lee-Yang Zeroes in the Four Dimensional Ising Model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"C.B. Lang, R. Kenna","submitted_at":"1993-11-20T11:42:44Z","abstract_excerpt":"The scaling behaviour of the edge of the Lee--Yang zeroes in the four dimensional Ising model is analyzed. This model is believed to belong to the same universality class as the $\\phi^4_4$ model which plays a central role in relativistic quantum field theory. While in the thermodynamic limit the scaling of the Yang--Lee edge is not modified by multiplicative logarithmic corrections, such corrections are manifest in the corresponding finite--size formulae. The asymptotic form for the density of zeroes which recovers the scaling behaviour of the susceptibility and the specific heat in the thermo"},"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/9311029","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1993-11-20T11:42:44Z","cross_cats_sorted":[],"title_canon_sha256":"8b85939448c410fb0e1a559e06a2b27cd00ef03f191ff37227cdf809b609fe9a","abstract_canon_sha256":"57cf318cbbf9ac152252b1da231b652701debfd80d8c9bd5459203076d874ce6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:17:45.982099Z","signature_b64":"ySIoDrlnKnVkkQ5jzYZBQUYj5Ch4+EhCmBar55C8GUjSgX3d8b3HVKnwKF3/NDR3xusoSPSrtAMn9dGT17X0AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dde217988a0f56c3ab064d08acbd917c6e0f19ceaaaff4f79984dd298cadf825","last_reissued_at":"2026-05-18T04:17:45.981704Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:17:45.981704Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Scaling and Density of Lee-Yang Zeroes in the Four Dimensional Ising Model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"C.B. Lang, R. Kenna","submitted_at":"1993-11-20T11:42:44Z","abstract_excerpt":"The scaling behaviour of the edge of the Lee--Yang zeroes in the four dimensional Ising model is analyzed. This model is believed to belong to the same universality class as the $\\phi^4_4$ model which plays a central role in relativistic quantum field theory. While in the thermodynamic limit the scaling of the Yang--Lee edge is not modified by multiplicative logarithmic corrections, such corrections are manifest in the corresponding finite--size formulae. The asymptotic form for the density of zeroes which recovers the scaling behaviour of the susceptibility and the specific heat in the thermo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9311029","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-lat/9311029","created_at":"2026-05-18T04:17:45.981763+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9311029v1","created_at":"2026-05-18T04:17:45.981763+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9311029","created_at":"2026-05-18T04:17:45.981763+00:00"},{"alias_kind":"pith_short_12","alias_value":"3XRBPGEKB5LM","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_16","alias_value":"3XRBPGEKB5LMHKYG","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_8","alias_value":"3XRBPGEK","created_at":"2026-05-18T12:25:47.102015+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2509.07250","citing_title":"Scale dependence improvement of the quartic scalar field thermal effective potential in the optimized perturbation theory","ref_index":71,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3XRBPGEKB5LMHKYGJUEKZPMRPR","json":"https://pith.science/pith/3XRBPGEKB5LMHKYGJUEKZPMRPR.json","graph_json":"https://pith.science/api/pith-number/3XRBPGEKB5LMHKYGJUEKZPMRPR/graph.json","events_json":"https://pith.science/api/pith-number/3XRBPGEKB5LMHKYGJUEKZPMRPR/events.json","paper":"https://pith.science/paper/3XRBPGEK"},"agent_actions":{"view_html":"https://pith.science/pith/3XRBPGEKB5LMHKYGJUEKZPMRPR","download_json":"https://pith.science/pith/3XRBPGEKB5LMHKYGJUEKZPMRPR.json","view_paper":"https://pith.science/paper/3XRBPGEK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/9311029&json=true","fetch_graph":"https://pith.science/api/pith-number/3XRBPGEKB5LMHKYGJUEKZPMRPR/graph.json","fetch_events":"https://pith.science/api/pith-number/3XRBPGEKB5LMHKYGJUEKZPMRPR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3XRBPGEKB5LMHKYGJUEKZPMRPR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3XRBPGEKB5LMHKYGJUEKZPMRPR/action/storage_attestation","attest_author":"https://pith.science/pith/3XRBPGEKB5LMHKYGJUEKZPMRPR/action/author_attestation","sign_citation":"https://pith.science/pith/3XRBPGEKB5LMHKYGJUEKZPMRPR/action/citation_signature","submit_replication":"https://pith.science/pith/3XRBPGEKB5LMHKYGJUEKZPMRPR/action/replication_record"}},"created_at":"2026-05-18T04:17:45.981763+00:00","updated_at":"2026-05-18T04:17:45.981763+00:00"}