{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:LGOCNKKT5AKVARJLAOJMKB6G2W","short_pith_number":"pith:LGOCNKKT","schema_version":"1.0","canonical_sha256":"599c26a953e81550452b0392c507c6d5a4841d449341de1371fbbd420cb47453","source":{"kind":"arxiv","id":"2010.05457","version":2},"attestation_state":"computed","paper":{"title":"Bottomonium suppression and elliptic flow using Heavy Quarkonium Quantum Dynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Ajaharul Islam, Michael Strickland","submitted_at":"2020-10-08T21:24:30Z","abstract_excerpt":"We introduce a framework called Heavy Quarkonium Quantum Dynamics (HQQD) which can be used to compute the dynamical suppression of heavy quarkonia propagating in the quark-gluon plasma using real-time in-medium quantum evolution. Using HQQD we compute large sets of real-time solutions to the Schr\\\"{o}dinger equation using a realistic in-medium complex-valued potential. We sample 2 million quarkonia wave packet trajectories and evolve them through the QGP using HQQD to obtain their survival probabilities. The computation is performed using three different HQQD model parameter sets in order to 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":"2010.05457","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-10-08T21:24:30Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"b37619f61cf509d9dd3c6f0727fac6b13c17b6b030943126a1ecf03913906a4a","abstract_canon_sha256":"ce1c4a036c04a12bbf750260f62a1d7b1bf210a8bdbaf855aeb9d25576bcd220"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:07:19.696506Z","signature_b64":"mMDFmOnbImJaSIYh0CgV3ngGaqnqYkM1QmStIWTq0guLOA99LF+1GJTIkHfX3rNWPPxJ5bXigi1qhzgcX/fwDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"599c26a953e81550452b0392c507c6d5a4841d449341de1371fbbd420cb47453","last_reissued_at":"2026-07-05T03:07:19.696035Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:07:19.696035Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Bottomonium suppression and elliptic flow using Heavy Quarkonium Quantum Dynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Ajaharul Islam, Michael Strickland","submitted_at":"2020-10-08T21:24:30Z","abstract_excerpt":"We introduce a framework called Heavy Quarkonium Quantum Dynamics (HQQD) which can be used to compute the dynamical suppression of heavy quarkonia propagating in the quark-gluon plasma using real-time in-medium quantum evolution. Using HQQD we compute large sets of real-time solutions to the Schr\\\"{o}dinger equation using a realistic in-medium complex-valued potential. We sample 2 million quarkonia wave packet trajectories and evolve them through the QGP using HQQD to obtain their survival probabilities. The computation is performed using three different HQQD model parameter sets in order to e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2010.05457","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/2010.05457/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":"2010.05457","created_at":"2026-07-05T03:07:19.696092+00:00"},{"alias_kind":"arxiv_version","alias_value":"2010.05457v2","created_at":"2026-07-05T03:07:19.696092+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2010.05457","created_at":"2026-07-05T03:07:19.696092+00:00"},{"alias_kind":"pith_short_12","alias_value":"LGOCNKKT5AKV","created_at":"2026-07-05T03:07:19.696092+00:00"},{"alias_kind":"pith_short_16","alias_value":"LGOCNKKT5AKVARJL","created_at":"2026-07-05T03:07:19.696092+00:00"},{"alias_kind":"pith_short_8","alias_value":"LGOCNKKT","created_at":"2026-07-05T03:07:19.696092+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"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":11,"is_internal_anchor":true},{"citing_arxiv_id":"2606.30959","citing_title":"A multi-differential constraint map for quarkonium suppression mechanisms in high-multiplicity pp and pPb collisions","ref_index":10,"is_internal_anchor":false},{"citing_arxiv_id":"2508.20995","citing_title":"Bottomonium transport in a strongly coupled quark-gluon plasma","ref_index":27,"is_internal_anchor":false},{"citing_arxiv_id":"2605.04558","citing_title":"Effects of event-by-event hydrodynamic fluctuations on bottomonium dynamics in Pb--Pb collisions at $\\sqrt{s_{NN}} = 5.02$ TeV","ref_index":21,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LGOCNKKT5AKVARJLAOJMKB6G2W","json":"https://pith.science/pith/LGOCNKKT5AKVARJLAOJMKB6G2W.json","graph_json":"https://pith.science/api/pith-number/LGOCNKKT5AKVARJLAOJMKB6G2W/graph.json","events_json":"https://pith.science/api/pith-number/LGOCNKKT5AKVARJLAOJMKB6G2W/events.json","paper":"https://pith.science/paper/LGOCNKKT"},"agent_actions":{"view_html":"https://pith.science/pith/LGOCNKKT5AKVARJLAOJMKB6G2W","download_json":"https://pith.science/pith/LGOCNKKT5AKVARJLAOJMKB6G2W.json","view_paper":"https://pith.science/paper/LGOCNKKT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2010.05457&json=true","fetch_graph":"https://pith.science/api/pith-number/LGOCNKKT5AKVARJLAOJMKB6G2W/graph.json","fetch_events":"https://pith.science/api/pith-number/LGOCNKKT5AKVARJLAOJMKB6G2W/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LGOCNKKT5AKVARJLAOJMKB6G2W/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LGOCNKKT5AKVARJLAOJMKB6G2W/action/storage_attestation","attest_author":"https://pith.science/pith/LGOCNKKT5AKVARJLAOJMKB6G2W/action/author_attestation","sign_citation":"https://pith.science/pith/LGOCNKKT5AKVARJLAOJMKB6G2W/action/citation_signature","submit_replication":"https://pith.science/pith/LGOCNKKT5AKVARJLAOJMKB6G2W/action/replication_record"}},"created_at":"2026-07-05T03:07:19.696092+00:00","updated_at":"2026-07-05T03:07:19.696092+00:00"}