{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:CL47QMXSWPZCA6UUZ4BVKQ4QNC","short_pith_number":"pith:CL47QMXS","schema_version":"1.0","canonical_sha256":"12f9f832f2b3f2207a94cf0355439068a1f4ad51d5f72e085367221b53d18ea6","source":{"kind":"arxiv","id":"2405.20280","version":2},"attestation_state":"computed","paper":{"title":"Quarkonium Polarization in Medium from Open Quantum Systems and Chromomagnetic Correlators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th","quant-ph"],"primary_cat":"hep-ph","authors_text":"Di-Lun Yang, Xiaojun Yao","submitted_at":"2024-05-30T17:33:38Z","abstract_excerpt":"We study the spin-dependent in-medium dynamics of quarkonia by using the potential nonrelativistic QCD (pNRQCD) and the open quantum system framework. We consider the pNRQCD Lagrangian valid up to the order $\\frac{r}{M^0}=r$ and $\\frac{r^0}{M}=\\frac{1}{M}$ in the double power counting. By considering the Markovian condition and applying the Wigner transformation upon the diagonal spin components of the quarkonium density matrix with the semiclassical expansion, we systematically derive the Boltzmann transport equation for quarkonia with polarization dependence in the quantum optical limit. Unl"},"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":"2405.20280","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-05-30T17:33:38Z","cross_cats_sorted":["nucl-th","quant-ph"],"title_canon_sha256":"f19218b2f50b1f614f244579fc9b2467eec59e514a61c35b031ebcdca043f428","abstract_canon_sha256":"fcf3df7cf2928030487aeafc5ed43ac42779042dff5cf952d89c3a1e77f10ab5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:28:50.707029Z","signature_b64":"YQjsaPcC+9V0W/SOihXkCCEqR65N2rTz2p4azVbI4f7pMT18PMPKkRfpDWuOSoygshoyO5qnrIVP6sMElnV0Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"12f9f832f2b3f2207a94cf0355439068a1f4ad51d5f72e085367221b53d18ea6","last_reissued_at":"2026-07-05T09:28:50.706533Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:28:50.706533Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quarkonium Polarization in Medium from Open Quantum Systems and Chromomagnetic Correlators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th","quant-ph"],"primary_cat":"hep-ph","authors_text":"Di-Lun Yang, Xiaojun Yao","submitted_at":"2024-05-30T17:33:38Z","abstract_excerpt":"We study the spin-dependent in-medium dynamics of quarkonia by using the potential nonrelativistic QCD (pNRQCD) and the open quantum system framework. We consider the pNRQCD Lagrangian valid up to the order $\\frac{r}{M^0}=r$ and $\\frac{r^0}{M}=\\frac{1}{M}$ in the double power counting. By considering the Markovian condition and applying the Wigner transformation upon the diagonal spin components of the quarkonium density matrix with the semiclassical expansion, we systematically derive the Boltzmann transport equation for quarkonia with polarization dependence in the quantum optical limit. Unl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2405.20280","kind":"arxiv","version":2},"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/2405.20280/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":"2405.20280","created_at":"2026-07-05T09:28:50.706609+00:00"},{"alias_kind":"arxiv_version","alias_value":"2405.20280v2","created_at":"2026-07-05T09:28:50.706609+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2405.20280","created_at":"2026-07-05T09:28:50.706609+00:00"},{"alias_kind":"pith_short_12","alias_value":"CL47QMXSWPZC","created_at":"2026-07-05T09:28:50.706609+00:00"},{"alias_kind":"pith_short_16","alias_value":"CL47QMXSWPZCA6UU","created_at":"2026-07-05T09:28:50.706609+00:00"},{"alias_kind":"pith_short_8","alias_value":"CL47QMXS","created_at":"2026-07-05T09:28:50.706609+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.30441","citing_title":"Factorizing quarkonium production matrix elements using effective field theory","ref_index":33,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CL47QMXSWPZCA6UUZ4BVKQ4QNC","json":"https://pith.science/pith/CL47QMXSWPZCA6UUZ4BVKQ4QNC.json","graph_json":"https://pith.science/api/pith-number/CL47QMXSWPZCA6UUZ4BVKQ4QNC/graph.json","events_json":"https://pith.science/api/pith-number/CL47QMXSWPZCA6UUZ4BVKQ4QNC/events.json","paper":"https://pith.science/paper/CL47QMXS"},"agent_actions":{"view_html":"https://pith.science/pith/CL47QMXSWPZCA6UUZ4BVKQ4QNC","download_json":"https://pith.science/pith/CL47QMXSWPZCA6UUZ4BVKQ4QNC.json","view_paper":"https://pith.science/paper/CL47QMXS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2405.20280&json=true","fetch_graph":"https://pith.science/api/pith-number/CL47QMXSWPZCA6UUZ4BVKQ4QNC/graph.json","fetch_events":"https://pith.science/api/pith-number/CL47QMXSWPZCA6UUZ4BVKQ4QNC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CL47QMXSWPZCA6UUZ4BVKQ4QNC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CL47QMXSWPZCA6UUZ4BVKQ4QNC/action/storage_attestation","attest_author":"https://pith.science/pith/CL47QMXSWPZCA6UUZ4BVKQ4QNC/action/author_attestation","sign_citation":"https://pith.science/pith/CL47QMXSWPZCA6UUZ4BVKQ4QNC/action/citation_signature","submit_replication":"https://pith.science/pith/CL47QMXSWPZCA6UUZ4BVKQ4QNC/action/replication_record"}},"created_at":"2026-07-05T09:28:50.706609+00:00","updated_at":"2026-07-05T09:28:50.706609+00:00"}