{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:MNF2MNM6AEAPEE625TTO753DI2","short_pith_number":"pith:MNF2MNM6","schema_version":"1.0","canonical_sha256":"634ba6359e0100f213daece6eff7634682e03e48a578d462cbbf9833f71e983e","source":{"kind":"arxiv","id":"2007.10211","version":2},"attestation_state":"computed","paper":{"title":"Bottomonium suppression and elliptic flow from real-time quantum evolution","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":"2020-07-20T15:51:14Z","abstract_excerpt":"We compute the suppression and elliptic flow of bottomonium using real-time solutions to the Schr\\\"{o}dinger equation with a realistic in-medium complex-valued potential. To model the initial production, we assume that, in the limit of heavy quark masses, the wave-function can be described by a lattice-smeared (Gaussian) Dirac delta wave-function. The resulting final-state quantum-mechanical overlaps provide the survival probability of all bottomonium eigenstates. Our results are in good agreement with available data for $R_{AA}$ as a function of $N_{\\rm part}$ and $p_T$ collected at $\\sqrt{s_"},"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":"2007.10211","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-07-20T15:51:14Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"239e985844fc315b7645ca54b8899fbc9eef52dda89d6f0a3a68c9d9a4856ac7","abstract_canon_sha256":"cd6aa54597acbfc348e35b8723eb541eb214f848bdda01474db2798faca1e057"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:53:21.288637Z","signature_b64":"g7wWcf28LxS/Yk4icFBF8W3Xlso3LFY1VObDue9XDlfaJJuBokA0fdowiKW5/b5td17mdZdaOoQMak9+SUVGAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"634ba6359e0100f213daece6eff7634682e03e48a578d462cbbf9833f71e983e","last_reissued_at":"2026-07-05T01:53:21.288140Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:53:21.288140Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Bottomonium suppression and elliptic flow from real-time quantum evolution","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":"2020-07-20T15:51:14Z","abstract_excerpt":"We compute the suppression and elliptic flow of bottomonium using real-time solutions to the Schr\\\"{o}dinger equation with a realistic in-medium complex-valued potential. To model the initial production, we assume that, in the limit of heavy quark masses, the wave-function can be described by a lattice-smeared (Gaussian) Dirac delta wave-function. The resulting final-state quantum-mechanical overlaps provide the survival probability of all bottomonium eigenstates. Our results are in good agreement with available data for $R_{AA}$ as a function of $N_{\\rm part}$ and $p_T$ collected at $\\sqrt{s_"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2007.10211","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/2007.10211/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":"2007.10211","created_at":"2026-07-05T01:53:21.288199+00:00"},{"alias_kind":"arxiv_version","alias_value":"2007.10211v2","created_at":"2026-07-05T01:53:21.288199+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2007.10211","created_at":"2026-07-05T01:53:21.288199+00:00"},{"alias_kind":"pith_short_12","alias_value":"MNF2MNM6AEAP","created_at":"2026-07-05T01:53:21.288199+00:00"},{"alias_kind":"pith_short_16","alias_value":"MNF2MNM6AEAPEE62","created_at":"2026-07-05T01:53:21.288199+00:00"},{"alias_kind":"pith_short_8","alias_value":"MNF2MNM6","created_at":"2026-07-05T01:53:21.288199+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"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":10,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MNF2MNM6AEAPEE625TTO753DI2","json":"https://pith.science/pith/MNF2MNM6AEAPEE625TTO753DI2.json","graph_json":"https://pith.science/api/pith-number/MNF2MNM6AEAPEE625TTO753DI2/graph.json","events_json":"https://pith.science/api/pith-number/MNF2MNM6AEAPEE625TTO753DI2/events.json","paper":"https://pith.science/paper/MNF2MNM6"},"agent_actions":{"view_html":"https://pith.science/pith/MNF2MNM6AEAPEE625TTO753DI2","download_json":"https://pith.science/pith/MNF2MNM6AEAPEE625TTO753DI2.json","view_paper":"https://pith.science/paper/MNF2MNM6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2007.10211&json=true","fetch_graph":"https://pith.science/api/pith-number/MNF2MNM6AEAPEE625TTO753DI2/graph.json","fetch_events":"https://pith.science/api/pith-number/MNF2MNM6AEAPEE625TTO753DI2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MNF2MNM6AEAPEE625TTO753DI2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MNF2MNM6AEAPEE625TTO753DI2/action/storage_attestation","attest_author":"https://pith.science/pith/MNF2MNM6AEAPEE625TTO753DI2/action/author_attestation","sign_citation":"https://pith.science/pith/MNF2MNM6AEAPEE625TTO753DI2/action/citation_signature","submit_replication":"https://pith.science/pith/MNF2MNM6AEAPEE625TTO753DI2/action/replication_record"}},"created_at":"2026-07-05T01:53:21.288199+00:00","updated_at":"2026-07-05T01:53:21.288199+00:00"}