{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:26S6C2HREXKHRZQSKNVMUBPXWW","short_pith_number":"pith:26S6C2HR","schema_version":"1.0","canonical_sha256":"d7a5e168f125d478e612536aca05f7b59426d51558196332e96383cca5e37db0","source":{"kind":"arxiv","id":"1811.07027","version":3},"attestation_state":"computed","paper":{"title":"Quarkonium In-Medium Transport Equation Derived from First Principles","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Thomas Mehen, Xiaojun Yao","submitted_at":"2018-11-16T20:34:52Z","abstract_excerpt":"We use the open quantum system formalism to study the dynamical in-medium evolution of quarkonium. The system of quarkonium is described by potential non-relativistic QCD while the environment is a weakly coupled quark-gluon plasma in local thermal equilibrium below the melting temperature of the quarkonium. Under the Markovian approximation, it is shown that the Lindblad equation leads to a Boltzmann transport equation if a Wigner transform is applied to the system density matrix. Our derivation illuminates how the microscopic time-reversibility of QCD is consistent with the time-irreversible"},"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":"1811.07027","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-11-16T20:34:52Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"5afe66a18706f02d9a1d7cf5d6a5926cf58ebf1d595ac4519c79daaca3a9197f","abstract_canon_sha256":"e8ba11aab92dd17f4deb629506bd5be7cc899416169b0b146dbac1ee37112b21"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:44:29.949262Z","signature_b64":"AaYqGrI0v1h7s2s1BG8DQCgYPWCfIrFIjmEsKChyM+VMPRqUfGCe1wHOcyFZcH6VOz9tM+J+ZnGT6qOoGrM0Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d7a5e168f125d478e612536aca05f7b59426d51558196332e96383cca5e37db0","last_reissued_at":"2026-05-17T23:44:29.948616Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:44:29.948616Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quarkonium In-Medium Transport Equation Derived from First Principles","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Thomas Mehen, Xiaojun Yao","submitted_at":"2018-11-16T20:34:52Z","abstract_excerpt":"We use the open quantum system formalism to study the dynamical in-medium evolution of quarkonium. The system of quarkonium is described by potential non-relativistic QCD while the environment is a weakly coupled quark-gluon plasma in local thermal equilibrium below the melting temperature of the quarkonium. Under the Markovian approximation, it is shown that the Lindblad equation leads to a Boltzmann transport equation if a Wigner transform is applied to the system density matrix. Our derivation illuminates how the microscopic time-reversibility of QCD is consistent with the time-irreversible"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.07027","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":"1811.07027","created_at":"2026-05-17T23:44:29.948732+00:00"},{"alias_kind":"arxiv_version","alias_value":"1811.07027v3","created_at":"2026-05-17T23:44:29.948732+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.07027","created_at":"2026-05-17T23:44:29.948732+00:00"},{"alias_kind":"pith_short_12","alias_value":"26S6C2HREXKH","created_at":"2026-05-18T12:31:59.375834+00:00"},{"alias_kind":"pith_short_16","alias_value":"26S6C2HREXKHRZQS","created_at":"2026-05-18T12:31:59.375834+00:00"},{"alias_kind":"pith_short_8","alias_value":"26S6C2HR","created_at":"2026-05-18T12:31:59.375834+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2604.26941","citing_title":"Schwinger-Keldysh Path Integral for Gauge theories","ref_index":179,"is_internal_anchor":true},{"citing_arxiv_id":"2508.20995","citing_title":"Bottomonium transport in a strongly coupled quark-gluon plasma","ref_index":28,"is_internal_anchor":true},{"citing_arxiv_id":"2512.01590","citing_title":"Directly computing Wigner functions for open quantum systems","ref_index":88,"is_internal_anchor":true},{"citing_arxiv_id":"2604.26941","citing_title":"Schwinger-Keldysh Path Integral for Gauge theories","ref_index":179,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/26S6C2HREXKHRZQSKNVMUBPXWW","json":"https://pith.science/pith/26S6C2HREXKHRZQSKNVMUBPXWW.json","graph_json":"https://pith.science/api/pith-number/26S6C2HREXKHRZQSKNVMUBPXWW/graph.json","events_json":"https://pith.science/api/pith-number/26S6C2HREXKHRZQSKNVMUBPXWW/events.json","paper":"https://pith.science/paper/26S6C2HR"},"agent_actions":{"view_html":"https://pith.science/pith/26S6C2HREXKHRZQSKNVMUBPXWW","download_json":"https://pith.science/pith/26S6C2HREXKHRZQSKNVMUBPXWW.json","view_paper":"https://pith.science/paper/26S6C2HR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1811.07027&json=true","fetch_graph":"https://pith.science/api/pith-number/26S6C2HREXKHRZQSKNVMUBPXWW/graph.json","fetch_events":"https://pith.science/api/pith-number/26S6C2HREXKHRZQSKNVMUBPXWW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/26S6C2HREXKHRZQSKNVMUBPXWW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/26S6C2HREXKHRZQSKNVMUBPXWW/action/storage_attestation","attest_author":"https://pith.science/pith/26S6C2HREXKHRZQSKNVMUBPXWW/action/author_attestation","sign_citation":"https://pith.science/pith/26S6C2HREXKHRZQSKNVMUBPXWW/action/citation_signature","submit_replication":"https://pith.science/pith/26S6C2HREXKHRZQSKNVMUBPXWW/action/replication_record"}},"created_at":"2026-05-17T23:44:29.948732+00:00","updated_at":"2026-05-17T23:44:29.948732+00:00"}