{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2000:JCGCG4BKMBOGX2LSBWRZO73VNZ","short_pith_number":"pith:JCGCG4BK","schema_version":"1.0","canonical_sha256":"488c23702a605c6be9720da3977f756e70b80c4c4a651f709951e1ec8cf6004c","source":{"kind":"arxiv","id":"hep-lat/0006009","version":3},"attestation_state":"computed","paper":{"title":"Extension to order $\\beta^{23}$ of the high-temperature expansions for the spin-1/2 Ising model on the simple-cubic and the body-centered-cubic lattices","license":"","headline":"","cross_cats":["cond-mat"],"primary_cat":"hep-lat","authors_text":"M. Comi (Phys. Dept. of Milano Bicocca Univ.), P. Butera","submitted_at":"2000-06-06T15:53:12Z","abstract_excerpt":"Using a renormalized linked-cluster-expansion method, we have extended to order $\\beta^{23}$ the high-temperature series for the susceptibility $\\chi$ and the second-moment correlation length $\\xi$ of the spin-1/2 Ising models on the sc and the bcc lattices. A study of these expansions yields updated direct estimates of universal parameters, such as exponents and amplitude ratios, which characterize the critical behavior of $\\chi$ and $\\xi$. Our best estimates for the inverse critical temperatures are\n $\\beta^{sc}_c=0.221654(1)$ and $\\beta^{bcc}_c=0.1573725(6)$. For the susceptibility exponent"},"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/0006009","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2000-06-06T15:53:12Z","cross_cats_sorted":["cond-mat"],"title_canon_sha256":"bddaca665028c20ac1c177ef4076aa1a427946a4c9e28617f01b5fd52cb53979","abstract_canon_sha256":"b031f19d8309e28d91a374e1f0ff02bbdeeac6ef66792fdb57e76292eb25754a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:39.420423Z","signature_b64":"T4AgbFGQfrHzhSWsM4OL3DEVd/2Hk6HNIxp2QCQkNIXqaCvInVkbJZIeCP6VVfbLy80OVEGF7uZSAc538Jc8Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"488c23702a605c6be9720da3977f756e70b80c4c4a651f709951e1ec8cf6004c","last_reissued_at":"2026-05-18T01:06:39.419710Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:39.419710Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Extension to order $\\beta^{23}$ of the high-temperature expansions for the spin-1/2 Ising model on the simple-cubic and the body-centered-cubic lattices","license":"","headline":"","cross_cats":["cond-mat"],"primary_cat":"hep-lat","authors_text":"M. Comi (Phys. Dept. of Milano Bicocca Univ.), P. Butera","submitted_at":"2000-06-06T15:53:12Z","abstract_excerpt":"Using a renormalized linked-cluster-expansion method, we have extended to order $\\beta^{23}$ the high-temperature series for the susceptibility $\\chi$ and the second-moment correlation length $\\xi$ of the spin-1/2 Ising models on the sc and the bcc lattices. A study of these expansions yields updated direct estimates of universal parameters, such as exponents and amplitude ratios, which characterize the critical behavior of $\\chi$ and $\\xi$. Our best estimates for the inverse critical temperatures are\n $\\beta^{sc}_c=0.221654(1)$ and $\\beta^{bcc}_c=0.1573725(6)$. For the susceptibility exponent"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0006009","kind":"arxiv","version":3},"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/0006009","created_at":"2026-05-18T01:06:39.419815+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0006009v3","created_at":"2026-05-18T01:06:39.419815+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0006009","created_at":"2026-05-18T01:06:39.419815+00:00"},{"alias_kind":"pith_short_12","alias_value":"JCGCG4BKMBOG","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_16","alias_value":"JCGCG4BKMBOGX2LS","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_8","alias_value":"JCGCG4BK","created_at":"2026-05-18T12:25:49.631198+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/JCGCG4BKMBOGX2LSBWRZO73VNZ","json":"https://pith.science/pith/JCGCG4BKMBOGX2LSBWRZO73VNZ.json","graph_json":"https://pith.science/api/pith-number/JCGCG4BKMBOGX2LSBWRZO73VNZ/graph.json","events_json":"https://pith.science/api/pith-number/JCGCG4BKMBOGX2LSBWRZO73VNZ/events.json","paper":"https://pith.science/paper/JCGCG4BK"},"agent_actions":{"view_html":"https://pith.science/pith/JCGCG4BKMBOGX2LSBWRZO73VNZ","download_json":"https://pith.science/pith/JCGCG4BKMBOGX2LSBWRZO73VNZ.json","view_paper":"https://pith.science/paper/JCGCG4BK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/0006009&json=true","fetch_graph":"https://pith.science/api/pith-number/JCGCG4BKMBOGX2LSBWRZO73VNZ/graph.json","fetch_events":"https://pith.science/api/pith-number/JCGCG4BKMBOGX2LSBWRZO73VNZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JCGCG4BKMBOGX2LSBWRZO73VNZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JCGCG4BKMBOGX2LSBWRZO73VNZ/action/storage_attestation","attest_author":"https://pith.science/pith/JCGCG4BKMBOGX2LSBWRZO73VNZ/action/author_attestation","sign_citation":"https://pith.science/pith/JCGCG4BKMBOGX2LSBWRZO73VNZ/action/citation_signature","submit_replication":"https://pith.science/pith/JCGCG4BKMBOGX2LSBWRZO73VNZ/action/replication_record"}},"created_at":"2026-05-18T01:06:39.419815+00:00","updated_at":"2026-05-18T01:06:39.419815+00:00"}