{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:H7R32O422CU3GWO7ATBT5ECINQ","short_pith_number":"pith:H7R32O42","schema_version":"1.0","canonical_sha256":"3fe3bd3b9ad0a9b359df04c33e90486c3991109d3cd7836dcfaf30336c159438","source":{"kind":"arxiv","id":"hep-lat/9901017","version":3},"attestation_state":"computed","paper":{"title":"Mesons Above The Deconfining Transition","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Nakamura, H. Matsufuru, I.-O. Stamatescu, M. Garcia Perez, O. Miyamura, QCD-TARO Collaboration: Ph. de Forcrand, S. Hioki, T. Hashimoto, T. Takaishi, T. Umeda","submitted_at":"1999-01-22T19:23:26Z","abstract_excerpt":"We analyze temporal and spatial meson correlators in quenched lattice QCD at T>0. Above T_c we find different masses and (spatial) screening masses, signals of plasma formation, and indication of persisting mesonic excitations."},"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/9901017","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1999-01-22T19:23:26Z","cross_cats_sorted":[],"title_canon_sha256":"fb776c264b70df8a13d8ea1b8997da9bba0b5ad55ef8ec54ddab9ec467e1675f","abstract_canon_sha256":"a7212db3597becac3a1ec9428ce5504b952cabc54d69110a9a0868cad280b513"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:47:11.517005Z","signature_b64":"14YAQbgkMChmC3LN6GdK4qLfAy8Y2h9httO/27aotCHixWkl1aZBsLS0TJikWWdjdnLdYPgng35ahPMtgqE8DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3fe3bd3b9ad0a9b359df04c33e90486c3991109d3cd7836dcfaf30336c159438","last_reissued_at":"2026-05-18T03:47:11.516309Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:47:11.516309Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Mesons Above The Deconfining Transition","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Nakamura, H. Matsufuru, I.-O. Stamatescu, M. Garcia Perez, O. Miyamura, QCD-TARO Collaboration: Ph. de Forcrand, S. Hioki, T. Hashimoto, T. Takaishi, T. Umeda","submitted_at":"1999-01-22T19:23:26Z","abstract_excerpt":"We analyze temporal and spatial meson correlators in quenched lattice QCD at T>0. Above T_c we find different masses and (spatial) screening masses, signals of plasma formation, and indication of persisting mesonic excitations."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9901017","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/9901017","created_at":"2026-05-18T03:47:11.516420+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9901017v3","created_at":"2026-05-18T03:47:11.516420+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9901017","created_at":"2026-05-18T03:47:11.516420+00:00"},{"alias_kind":"pith_short_12","alias_value":"H7R32O422CU3","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_16","alias_value":"H7R32O422CU3GWO7","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_8","alias_value":"H7R32O42","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/H7R32O422CU3GWO7ATBT5ECINQ","json":"https://pith.science/pith/H7R32O422CU3GWO7ATBT5ECINQ.json","graph_json":"https://pith.science/api/pith-number/H7R32O422CU3GWO7ATBT5ECINQ/graph.json","events_json":"https://pith.science/api/pith-number/H7R32O422CU3GWO7ATBT5ECINQ/events.json","paper":"https://pith.science/paper/H7R32O42"},"agent_actions":{"view_html":"https://pith.science/pith/H7R32O422CU3GWO7ATBT5ECINQ","download_json":"https://pith.science/pith/H7R32O422CU3GWO7ATBT5ECINQ.json","view_paper":"https://pith.science/paper/H7R32O42","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/9901017&json=true","fetch_graph":"https://pith.science/api/pith-number/H7R32O422CU3GWO7ATBT5ECINQ/graph.json","fetch_events":"https://pith.science/api/pith-number/H7R32O422CU3GWO7ATBT5ECINQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/H7R32O422CU3GWO7ATBT5ECINQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/H7R32O422CU3GWO7ATBT5ECINQ/action/storage_attestation","attest_author":"https://pith.science/pith/H7R32O422CU3GWO7ATBT5ECINQ/action/author_attestation","sign_citation":"https://pith.science/pith/H7R32O422CU3GWO7ATBT5ECINQ/action/citation_signature","submit_replication":"https://pith.science/pith/H7R32O422CU3GWO7ATBT5ECINQ/action/replication_record"}},"created_at":"2026-05-18T03:47:11.516420+00:00","updated_at":"2026-05-18T03:47:11.516420+00:00"}