{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:IVV55TBFDD4NIPSYNBOLU3DCUQ","short_pith_number":"pith:IVV55TBF","schema_version":"1.0","canonical_sha256":"456bdecc2518f8d43e58685cba6c62a412e01abdc4df446538454f909686dcee","source":{"kind":"arxiv","id":"1505.06616","version":1},"attestation_state":"computed","paper":{"title":"The Charmonium Potential at Non-Zero Temperature","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Chris Allton, Jon-Ivar Skullerud, Pietro Giudice, Wynne Evans","submitted_at":"2015-05-25T13:11:46Z","abstract_excerpt":"The potential between charm and anti-charm quarks is calculated non-perturbatively using physical, rather than static quarks at temperatures on both sides of the deconfinement transition $T_{\\rm C}$, using a lattice simulation with 2+1 dynamical quark flavours. We used the HAL QCD time-dependent method, originally developed for inter-nucleon potentials. Our lattices are anisotropic, with temporal lattice spacing less than the spatial one which enhances the information content of our correlators at each temperature. Local-extended charmonium correlators were calculated efficiently by contractin"},"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":"1505.06616","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-05-25T13:11:46Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"24ff8831dc06b473e87ae3a485336dc472cc53966aae8d03ba339c9f0ef41d4e","abstract_canon_sha256":"f57d12b2c7c82e9a21c9103894c39c7ea03247959d50b4ced9a5d0df85361630"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:03:44.487768Z","signature_b64":"XbVIQlLuatNKldpuHj7FeoRFNK5DCiB56yWuIxcRq/FWBy3ZEyP+O/HsyV1iFLh0PSrSVsPs68lZu5vkgluHCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"456bdecc2518f8d43e58685cba6c62a412e01abdc4df446538454f909686dcee","last_reissued_at":"2026-05-18T02:03:44.487172Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:03:44.487172Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Charmonium Potential at Non-Zero Temperature","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Chris Allton, Jon-Ivar Skullerud, Pietro Giudice, Wynne Evans","submitted_at":"2015-05-25T13:11:46Z","abstract_excerpt":"The potential between charm and anti-charm quarks is calculated non-perturbatively using physical, rather than static quarks at temperatures on both sides of the deconfinement transition $T_{\\rm C}$, using a lattice simulation with 2+1 dynamical quark flavours. We used the HAL QCD time-dependent method, originally developed for inter-nucleon potentials. Our lattices are anisotropic, with temporal lattice spacing less than the spatial one which enhances the information content of our correlators at each temperature. Local-extended charmonium correlators were calculated efficiently by contractin"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.06616","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":"1505.06616","created_at":"2026-05-18T02:03:44.487257+00:00"},{"alias_kind":"arxiv_version","alias_value":"1505.06616v1","created_at":"2026-05-18T02:03:44.487257+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.06616","created_at":"2026-05-18T02:03:44.487257+00:00"},{"alias_kind":"pith_short_12","alias_value":"IVV55TBFDD4N","created_at":"2026-05-18T12:29:25.134429+00:00"},{"alias_kind":"pith_short_16","alias_value":"IVV55TBFDD4NIPSY","created_at":"2026-05-18T12:29:25.134429+00:00"},{"alias_kind":"pith_short_8","alias_value":"IVV55TBF","created_at":"2026-05-18T12:29:25.134429+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/IVV55TBFDD4NIPSYNBOLU3DCUQ","json":"https://pith.science/pith/IVV55TBFDD4NIPSYNBOLU3DCUQ.json","graph_json":"https://pith.science/api/pith-number/IVV55TBFDD4NIPSYNBOLU3DCUQ/graph.json","events_json":"https://pith.science/api/pith-number/IVV55TBFDD4NIPSYNBOLU3DCUQ/events.json","paper":"https://pith.science/paper/IVV55TBF"},"agent_actions":{"view_html":"https://pith.science/pith/IVV55TBFDD4NIPSYNBOLU3DCUQ","download_json":"https://pith.science/pith/IVV55TBFDD4NIPSYNBOLU3DCUQ.json","view_paper":"https://pith.science/paper/IVV55TBF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1505.06616&json=true","fetch_graph":"https://pith.science/api/pith-number/IVV55TBFDD4NIPSYNBOLU3DCUQ/graph.json","fetch_events":"https://pith.science/api/pith-number/IVV55TBFDD4NIPSYNBOLU3DCUQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IVV55TBFDD4NIPSYNBOLU3DCUQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IVV55TBFDD4NIPSYNBOLU3DCUQ/action/storage_attestation","attest_author":"https://pith.science/pith/IVV55TBFDD4NIPSYNBOLU3DCUQ/action/author_attestation","sign_citation":"https://pith.science/pith/IVV55TBFDD4NIPSYNBOLU3DCUQ/action/citation_signature","submit_replication":"https://pith.science/pith/IVV55TBFDD4NIPSYNBOLU3DCUQ/action/replication_record"}},"created_at":"2026-05-18T02:03:44.487257+00:00","updated_at":"2026-05-18T02:03:44.487257+00:00"}