{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:BWSPTW7ZXDS42DLMP54LHP6JUW","short_pith_number":"pith:BWSPTW7Z","schema_version":"1.0","canonical_sha256":"0da4f9dbf9b8e5cd0d6c7f78b3bfc9a5a4781a26d9d37f4761cb53b19cfae5d7","source":{"kind":"arxiv","id":"2407.01064","version":3},"attestation_state":"computed","paper":{"title":"Magnetic Polarisability of Octet Baryons via Lattice QCD","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"(2) Trinity College), Derek Leinweber (1) ((1) University of Adelaide, Ryan Bignell (2), Thomas Kabelitz (1), Waseem Kamleh (1)","submitted_at":"2024-07-01T08:13:05Z","abstract_excerpt":"Drawing on recent advances in lattice-QCD background-field techniques, the magnetic polarisability of octet baryons is calculated from the first principles of QCD. The results are presented in the context of new constituent quark-model calculations providing a framework for understanding the lattice results and a direct comparison with simulation results at unphysical quark masses. Using smeared quark sources, low-lying Laplacian eigenmode projection and final-state Landau mode projection, considerable attention is devoted to ensuring single-state isolation in the lattice correlation functions"},"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":"2407.01064","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-lat","submitted_at":"2024-07-01T08:13:05Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"027d89febc3b0ca01c2ad98fa7f952ca792e83ede15eefc4b4c8e5415573d184","abstract_canon_sha256":"0587a4a1a90019e9e122bd236f2ef82e80b3d80353fc9775675a4c9f3b927514"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:23:53.604771Z","signature_b64":"2uQgver0SObc8uqEsHNNXQD4c+SQNJhA84FdgTFrFBIvtM/fRBBGP/cNLb+ZzdSnBIEXxZh+Hzwc6/D674ilBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0da4f9dbf9b8e5cd0d6c7f78b3bfc9a5a4781a26d9d37f4761cb53b19cfae5d7","last_reissued_at":"2026-07-05T09:23:53.604274Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:23:53.604274Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Magnetic Polarisability of Octet Baryons via Lattice QCD","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"(2) Trinity College), Derek Leinweber (1) ((1) University of Adelaide, Ryan Bignell (2), Thomas Kabelitz (1), Waseem Kamleh (1)","submitted_at":"2024-07-01T08:13:05Z","abstract_excerpt":"Drawing on recent advances in lattice-QCD background-field techniques, the magnetic polarisability of octet baryons is calculated from the first principles of QCD. The results are presented in the context of new constituent quark-model calculations providing a framework for understanding the lattice results and a direct comparison with simulation results at unphysical quark masses. Using smeared quark sources, low-lying Laplacian eigenmode projection and final-state Landau mode projection, considerable attention is devoted to ensuring single-state isolation in the lattice correlation functions"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2407.01064","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2407.01064/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":"2407.01064","created_at":"2026-07-05T09:23:53.604350+00:00"},{"alias_kind":"arxiv_version","alias_value":"2407.01064v3","created_at":"2026-07-05T09:23:53.604350+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2407.01064","created_at":"2026-07-05T09:23:53.604350+00:00"},{"alias_kind":"pith_short_12","alias_value":"BWSPTW7ZXDS4","created_at":"2026-07-05T09:23:53.604350+00:00"},{"alias_kind":"pith_short_16","alias_value":"BWSPTW7ZXDS42DLM","created_at":"2026-07-05T09:23:53.604350+00:00"},{"alias_kind":"pith_short_8","alias_value":"BWSPTW7Z","created_at":"2026-07-05T09:23:53.604350+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.08960","citing_title":"Magnetic polarisability of octet baryons near the physical quark-mass point","ref_index":8,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BWSPTW7ZXDS42DLMP54LHP6JUW","json":"https://pith.science/pith/BWSPTW7ZXDS42DLMP54LHP6JUW.json","graph_json":"https://pith.science/api/pith-number/BWSPTW7ZXDS42DLMP54LHP6JUW/graph.json","events_json":"https://pith.science/api/pith-number/BWSPTW7ZXDS42DLMP54LHP6JUW/events.json","paper":"https://pith.science/paper/BWSPTW7Z"},"agent_actions":{"view_html":"https://pith.science/pith/BWSPTW7ZXDS42DLMP54LHP6JUW","download_json":"https://pith.science/pith/BWSPTW7ZXDS42DLMP54LHP6JUW.json","view_paper":"https://pith.science/paper/BWSPTW7Z","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2407.01064&json=true","fetch_graph":"https://pith.science/api/pith-number/BWSPTW7ZXDS42DLMP54LHP6JUW/graph.json","fetch_events":"https://pith.science/api/pith-number/BWSPTW7ZXDS42DLMP54LHP6JUW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BWSPTW7ZXDS42DLMP54LHP6JUW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BWSPTW7ZXDS42DLMP54LHP6JUW/action/storage_attestation","attest_author":"https://pith.science/pith/BWSPTW7ZXDS42DLMP54LHP6JUW/action/author_attestation","sign_citation":"https://pith.science/pith/BWSPTW7ZXDS42DLMP54LHP6JUW/action/citation_signature","submit_replication":"https://pith.science/pith/BWSPTW7ZXDS42DLMP54LHP6JUW/action/replication_record"}},"created_at":"2026-07-05T09:23:53.604350+00:00","updated_at":"2026-07-05T09:23:53.604350+00:00"}