{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:WSBHQ2M3X6CYRAIUSKARBW6DRP","short_pith_number":"pith:WSBHQ2M3","schema_version":"1.0","canonical_sha256":"b48278699bbf85888114928110dbc38bcccfdd2104c8f2573a105bba7b0014c3","source":{"kind":"arxiv","id":"1906.00035","version":4},"attestation_state":"computed","paper":{"title":"Improved Gauss law model and in-medium heavy quarkonium at finite density and velocity","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Alexander Rothkopf, David Lafferty","submitted_at":"2019-05-31T19:01:05Z","abstract_excerpt":"We explore the in-medium properties of heavy-quarkonium states at finite baryo-chemical potential and finite transverse momentum based on a modern complex-valued potential model. Our starting point is a novel, rigorous derivation of the generalized Gauss law for in-medium quarkonium, combining the non-perturbative physics of the vacuum bound state with a weak coupling description of the medium degrees of freedom. Its relation to previous models in the literature is discussed. We show that our approach is able to reproduce the complex lattice QCD heavy quark potential even in the non-perturbati"},"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":"1906.00035","kind":"arxiv","version":4},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2019-05-31T19:01:05Z","cross_cats_sorted":["hep-lat","nucl-th"],"title_canon_sha256":"490549d9ee36220068c0bfb5656043b6158e0c7b0b97059b2ce9e52422a01df6","abstract_canon_sha256":"127adf82c5df8f37c07f87ca7cfeb6548c58e319105eee450d308506b5bd94d0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:47:16.858226Z","signature_b64":"2StAVWiiZiJZSgqVtiPzyUkda6tEj8du8KkCRZsgfN3VYtgFdfx01shDqrIw9+1N87SwURIMG9qLNiTVZvn9Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b48278699bbf85888114928110dbc38bcccfdd2104c8f2573a105bba7b0014c3","last_reissued_at":"2026-07-05T00:47:16.857652Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:47:16.857652Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Improved Gauss law model and in-medium heavy quarkonium at finite density and velocity","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Alexander Rothkopf, David Lafferty","submitted_at":"2019-05-31T19:01:05Z","abstract_excerpt":"We explore the in-medium properties of heavy-quarkonium states at finite baryo-chemical potential and finite transverse momentum based on a modern complex-valued potential model. Our starting point is a novel, rigorous derivation of the generalized Gauss law for in-medium quarkonium, combining the non-perturbative physics of the vacuum bound state with a weak coupling description of the medium degrees of freedom. Its relation to previous models in the literature is discussed. We show that our approach is able to reproduce the complex lattice QCD heavy quark potential even in the non-perturbati"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1906.00035","kind":"arxiv","version":4},"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/1906.00035/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":"1906.00035","created_at":"2026-07-05T00:47:16.857712+00:00"},{"alias_kind":"arxiv_version","alias_value":"1906.00035v4","created_at":"2026-07-05T00:47:16.857712+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1906.00035","created_at":"2026-07-05T00:47:16.857712+00:00"},{"alias_kind":"pith_short_12","alias_value":"WSBHQ2M3X6CY","created_at":"2026-07-05T00:47:16.857712+00:00"},{"alias_kind":"pith_short_16","alias_value":"WSBHQ2M3X6CYRAIU","created_at":"2026-07-05T00:47:16.857712+00:00"},{"alias_kind":"pith_short_8","alias_value":"WSBHQ2M3","created_at":"2026-07-05T00:47:16.857712+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.06191","citing_title":"Bottomonium production in an open quantum system approach with interactions from lattice quantum chromodynamic","ref_index":31,"is_internal_anchor":true},{"citing_arxiv_id":"2604.10889","citing_title":"Heavy-quark transport across the QCD crossover driven by a lattice-constrained in-medium potential","ref_index":26,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WSBHQ2M3X6CYRAIUSKARBW6DRP","json":"https://pith.science/pith/WSBHQ2M3X6CYRAIUSKARBW6DRP.json","graph_json":"https://pith.science/api/pith-number/WSBHQ2M3X6CYRAIUSKARBW6DRP/graph.json","events_json":"https://pith.science/api/pith-number/WSBHQ2M3X6CYRAIUSKARBW6DRP/events.json","paper":"https://pith.science/paper/WSBHQ2M3"},"agent_actions":{"view_html":"https://pith.science/pith/WSBHQ2M3X6CYRAIUSKARBW6DRP","download_json":"https://pith.science/pith/WSBHQ2M3X6CYRAIUSKARBW6DRP.json","view_paper":"https://pith.science/paper/WSBHQ2M3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1906.00035&json=true","fetch_graph":"https://pith.science/api/pith-number/WSBHQ2M3X6CYRAIUSKARBW6DRP/graph.json","fetch_events":"https://pith.science/api/pith-number/WSBHQ2M3X6CYRAIUSKARBW6DRP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WSBHQ2M3X6CYRAIUSKARBW6DRP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WSBHQ2M3X6CYRAIUSKARBW6DRP/action/storage_attestation","attest_author":"https://pith.science/pith/WSBHQ2M3X6CYRAIUSKARBW6DRP/action/author_attestation","sign_citation":"https://pith.science/pith/WSBHQ2M3X6CYRAIUSKARBW6DRP/action/citation_signature","submit_replication":"https://pith.science/pith/WSBHQ2M3X6CYRAIUSKARBW6DRP/action/replication_record"}},"created_at":"2026-07-05T00:47:16.857712+00:00","updated_at":"2026-07-05T00:47:16.857712+00:00"}