{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:7EI46FASOHDQ544S4OCKMY4LPI","short_pith_number":"pith:7EI46FAS","schema_version":"1.0","canonical_sha256":"f911cf141271c70ef392e384a6638b7a0bd6137b0edcd2a3322a2e627d09019a","source":{"kind":"arxiv","id":"1311.3759","version":1},"attestation_state":"computed","paper":{"title":"Towards the continuum limit in transport coefficient computations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Francis, H. Ohno, M. Laine, M. M\\\"uller, O. Kaczmarek, T. Neuhaus","submitted_at":"2013-11-15T07:55:42Z","abstract_excerpt":"The analytic continuation needed for the extraction of transport coefficients necessitates in principle a continuous function of the Euclidean time variable. We report on progress towards achieving the continuum limit for 2-point correlator measurements in thermal SU(3) gauge theory, with specific attention paid to scale setting. In particular, we improve upon the determination of the critical lattice coupling and the critical temperature of pure SU(3) gauge theory, estimating r0*Tc ~ 0.7470(7) after a continuum extrapolation. As an application the determination of the heavy quark momentum dif"},"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":"1311.3759","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-11-15T07:55:42Z","cross_cats_sorted":[],"title_canon_sha256":"dfd75a18c42ee020fa918f5b3c10a79dc4a8f674ef2817db5cd6e0487daac077","abstract_canon_sha256":"aa47932bbe7e8c0c773adcc1ee6df553ef8ec8520e6e450b4b6958eccd9c2af9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:07:03.098824Z","signature_b64":"0RgcLQsgRUuReGPtH1Q9fhSOre32fVSwFtYxsFZmHvekyEMCn9/2yAWthdcp7wnb0kwLX/tGG/4Q/tIUCvCDAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f911cf141271c70ef392e384a6638b7a0bd6137b0edcd2a3322a2e627d09019a","last_reissued_at":"2026-05-18T03:07:03.098387Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:07:03.098387Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Towards the continuum limit in transport coefficient computations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Francis, H. Ohno, M. Laine, M. M\\\"uller, O. Kaczmarek, T. Neuhaus","submitted_at":"2013-11-15T07:55:42Z","abstract_excerpt":"The analytic continuation needed for the extraction of transport coefficients necessitates in principle a continuous function of the Euclidean time variable. We report on progress towards achieving the continuum limit for 2-point correlator measurements in thermal SU(3) gauge theory, with specific attention paid to scale setting. In particular, we improve upon the determination of the critical lattice coupling and the critical temperature of pure SU(3) gauge theory, estimating r0*Tc ~ 0.7470(7) after a continuum extrapolation. As an application the determination of the heavy quark momentum dif"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.3759","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":"1311.3759","created_at":"2026-05-18T03:07:03.098451+00:00"},{"alias_kind":"arxiv_version","alias_value":"1311.3759v1","created_at":"2026-05-18T03:07:03.098451+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.3759","created_at":"2026-05-18T03:07:03.098451+00:00"},{"alias_kind":"pith_short_12","alias_value":"7EI46FASOHDQ","created_at":"2026-05-18T12:27:36.564083+00:00"},{"alias_kind":"pith_short_16","alias_value":"7EI46FASOHDQ544S","created_at":"2026-05-18T12:27:36.564083+00:00"},{"alias_kind":"pith_short_8","alias_value":"7EI46FAS","created_at":"2026-05-18T12:27:36.564083+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/7EI46FASOHDQ544S4OCKMY4LPI","json":"https://pith.science/pith/7EI46FASOHDQ544S4OCKMY4LPI.json","graph_json":"https://pith.science/api/pith-number/7EI46FASOHDQ544S4OCKMY4LPI/graph.json","events_json":"https://pith.science/api/pith-number/7EI46FASOHDQ544S4OCKMY4LPI/events.json","paper":"https://pith.science/paper/7EI46FAS"},"agent_actions":{"view_html":"https://pith.science/pith/7EI46FASOHDQ544S4OCKMY4LPI","download_json":"https://pith.science/pith/7EI46FASOHDQ544S4OCKMY4LPI.json","view_paper":"https://pith.science/paper/7EI46FAS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1311.3759&json=true","fetch_graph":"https://pith.science/api/pith-number/7EI46FASOHDQ544S4OCKMY4LPI/graph.json","fetch_events":"https://pith.science/api/pith-number/7EI46FASOHDQ544S4OCKMY4LPI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7EI46FASOHDQ544S4OCKMY4LPI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7EI46FASOHDQ544S4OCKMY4LPI/action/storage_attestation","attest_author":"https://pith.science/pith/7EI46FASOHDQ544S4OCKMY4LPI/action/author_attestation","sign_citation":"https://pith.science/pith/7EI46FASOHDQ544S4OCKMY4LPI/action/citation_signature","submit_replication":"https://pith.science/pith/7EI46FASOHDQ544S4OCKMY4LPI/action/replication_record"}},"created_at":"2026-05-18T03:07:03.098451+00:00","updated_at":"2026-05-18T03:07:03.098451+00:00"}