{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:XKAQH7N3GASBTPBPWMDZRXKQNT","short_pith_number":"pith:XKAQH7N3","schema_version":"1.0","canonical_sha256":"ba8103fdbb302419bc2fb30798dd506cebdaed520a9330db19cf6acb2e42de62","source":{"kind":"arxiv","id":"1511.00032","version":1},"attestation_state":"computed","paper":{"title":"Static quark-antiquark pair free energy and screening masses: continuum results at the QCD physical point","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Attila Pasztor, Csaba Torok, Kalman K. Szabo, Sandor D. Katz, Szabolcs Borsanyi, Zoltan Fodor","submitted_at":"2015-10-30T21:21:15Z","abstract_excerpt":"We study the correlators of Polyakov loops, and the corresponding gauge invariant free energy of a static quark-antiquark pair in 2+1 flavor QCD at finite temperature. Our simulations were carried out on $N_t$ = 6, 8, 10, 12, 16 lattices using a Symanzik improved gauge action and a stout improved staggered action with physical quark masses. The free energies calculated from the Polyakov loop correlators are extrapolated to the continuum limit. For the free energies we use a two step renormalization procedure that only uses data at finite temperature. We also measure correlators with definite E"},"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":"1511.00032","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-10-30T21:21:15Z","cross_cats_sorted":[],"title_canon_sha256":"b7facf7c27bd5c218e95ee346bd13d575a7e8b1e109d2c89b69a90c82d2e3d4a","abstract_canon_sha256":"bbbfadf76bfdaa9a2644c806723b5014869b2fabc7772e5c51ed50bffc3c9dcb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:28:13.531568Z","signature_b64":"N5SGFU61h+7X8AjVT0pHC9Hb5tAXE2upYm4SGyRWzTMYrWpg/mitLVJi/eVsMTLXDk0T2IADDangN/FWGmBWDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ba8103fdbb302419bc2fb30798dd506cebdaed520a9330db19cf6acb2e42de62","last_reissued_at":"2026-05-18T01:28:13.530820Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:28:13.530820Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Static quark-antiquark pair free energy and screening masses: continuum results at the QCD physical point","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Attila Pasztor, Csaba Torok, Kalman K. Szabo, Sandor D. Katz, Szabolcs Borsanyi, Zoltan Fodor","submitted_at":"2015-10-30T21:21:15Z","abstract_excerpt":"We study the correlators of Polyakov loops, and the corresponding gauge invariant free energy of a static quark-antiquark pair in 2+1 flavor QCD at finite temperature. Our simulations were carried out on $N_t$ = 6, 8, 10, 12, 16 lattices using a Symanzik improved gauge action and a stout improved staggered action with physical quark masses. The free energies calculated from the Polyakov loop correlators are extrapolated to the continuum limit. For the free energies we use a two step renormalization procedure that only uses data at finite temperature. We also measure correlators with definite E"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.00032","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":"1511.00032","created_at":"2026-05-18T01:28:13.530932+00:00"},{"alias_kind":"arxiv_version","alias_value":"1511.00032v1","created_at":"2026-05-18T01:28:13.530932+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.00032","created_at":"2026-05-18T01:28:13.530932+00:00"},{"alias_kind":"pith_short_12","alias_value":"XKAQH7N3GASB","created_at":"2026-05-18T12:29:50.041715+00:00"},{"alias_kind":"pith_short_16","alias_value":"XKAQH7N3GASBTPBP","created_at":"2026-05-18T12:29:50.041715+00:00"},{"alias_kind":"pith_short_8","alias_value":"XKAQH7N3","created_at":"2026-05-18T12:29:50.041715+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/XKAQH7N3GASBTPBPWMDZRXKQNT","json":"https://pith.science/pith/XKAQH7N3GASBTPBPWMDZRXKQNT.json","graph_json":"https://pith.science/api/pith-number/XKAQH7N3GASBTPBPWMDZRXKQNT/graph.json","events_json":"https://pith.science/api/pith-number/XKAQH7N3GASBTPBPWMDZRXKQNT/events.json","paper":"https://pith.science/paper/XKAQH7N3"},"agent_actions":{"view_html":"https://pith.science/pith/XKAQH7N3GASBTPBPWMDZRXKQNT","download_json":"https://pith.science/pith/XKAQH7N3GASBTPBPWMDZRXKQNT.json","view_paper":"https://pith.science/paper/XKAQH7N3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1511.00032&json=true","fetch_graph":"https://pith.science/api/pith-number/XKAQH7N3GASBTPBPWMDZRXKQNT/graph.json","fetch_events":"https://pith.science/api/pith-number/XKAQH7N3GASBTPBPWMDZRXKQNT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XKAQH7N3GASBTPBPWMDZRXKQNT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XKAQH7N3GASBTPBPWMDZRXKQNT/action/storage_attestation","attest_author":"https://pith.science/pith/XKAQH7N3GASBTPBPWMDZRXKQNT/action/author_attestation","sign_citation":"https://pith.science/pith/XKAQH7N3GASBTPBPWMDZRXKQNT/action/citation_signature","submit_replication":"https://pith.science/pith/XKAQH7N3GASBTPBPWMDZRXKQNT/action/replication_record"}},"created_at":"2026-05-18T01:28:13.530932+00:00","updated_at":"2026-05-18T01:28:13.530932+00:00"}