{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2020:6NTPVDF7WVMKBOPU2YMQNZYC66","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"28d991db87c73899a7c6d766ea85cbbcc22882d941b55b14add732f3fa38ae89","cross_cats_sorted":["nucl-ex","nucl-th","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-12-02T14:34:28Z","title_canon_sha256":"f4ecf9c2bb6fc1b36c4795d48bd668cbac49cce5f87099795d5a8ee17690f535"},"schema_version":"1.0","source":{"id":"2012.01240","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2012.01240","created_at":"2026-07-05T05:31:41Z"},{"alias_kind":"arxiv_version","alias_value":"2012.01240v2","created_at":"2026-07-05T05:31:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2012.01240","created_at":"2026-07-05T05:31:41Z"},{"alias_kind":"pith_short_12","alias_value":"6NTPVDF7WVMK","created_at":"2026-07-05T05:31:41Z"},{"alias_kind":"pith_short_16","alias_value":"6NTPVDF7WVMKBOPU","created_at":"2026-07-05T05:31:41Z"},{"alias_kind":"pith_short_8","alias_value":"6NTPVDF7","created_at":"2026-07-05T05:31:41Z"}],"graph_snapshots":[{"event_id":"sha256:26d9dc2ba0b2b9d417cdadb8419908bff8e41629e3dcf786bb501892aa6acf17","target":"graph","created_at":"2026-07-05T05:31:41Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2012.01240/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We solve the Lindblad equation describing the Brownian motion of a Coulombic heavy quark-antiquark pair in a strongly coupled quark-gluon plasma using the highly efficient Monte Carlo wave-function method. The Lindblad equation has been derived in the framework of pNRQCD and fully accounts for the quantum and non-Abelian nature of the system. The hydrodynamics of the plasma is realistically implemented through a 3+1D dissipative hydrodynamics code. We compute the bottomonium nuclear modification factor and compare with the most recent LHC data. The computation does not rely on any free paramet","authors_text":"Antonio Vairo, Johannes Heinrich Weber, Michael Strickland, Miguel \\'Angel Escobedo, Nora Brambilla, Peter Vander Griend","cross_cats":["nucl-ex","nucl-th","physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-12-02T14:34:28Z","title":"Bottomonium suppression in an open quantum system using the quantum trajectories method"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2012.01240","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:8c7751cebc0aced0d0efa926b5e69d58f9e2629fa49e402f674c58d09244452b","target":"record","created_at":"2026-07-05T05:31:41Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"28d991db87c73899a7c6d766ea85cbbcc22882d941b55b14add732f3fa38ae89","cross_cats_sorted":["nucl-ex","nucl-th","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-12-02T14:34:28Z","title_canon_sha256":"f4ecf9c2bb6fc1b36c4795d48bd668cbac49cce5f87099795d5a8ee17690f535"},"schema_version":"1.0","source":{"id":"2012.01240","kind":"arxiv","version":2}},"canonical_sha256":"f366fa8cbfb558a0b9f4d61906e702f7b933aea3c7038b36b7813c1c8065a5f9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f366fa8cbfb558a0b9f4d61906e702f7b933aea3c7038b36b7813c1c8065a5f9","first_computed_at":"2026-07-05T05:31:41.023593Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:31:41.023593Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"AM4Fih59mIGoyVZyFGNstkrxJFHaDjihLAuJj4/I0FicoPYvAPYZM2TbHZdeB7rrK6A/PubC9eHM7vR33mTkCg==","signature_status":"signed_v1","signed_at":"2026-07-05T05:31:41.024025Z","signed_message":"canonical_sha256_bytes"},"source_id":"2012.01240","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8c7751cebc0aced0d0efa926b5e69d58f9e2629fa49e402f674c58d09244452b","sha256:26d9dc2ba0b2b9d417cdadb8419908bff8e41629e3dcf786bb501892aa6acf17"],"state_sha256":"12b4688fdf66b7d05c16c1f91497a7d959d8fbb044649a61e1296d628ef79e33"}