{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:RSPE4KTJ5ZOHLJOUHTRTMYV7VB","short_pith_number":"pith:RSPE4KTJ","schema_version":"1.0","canonical_sha256":"8c9e4e2a69ee5c75a5d43ce33662bfa86e64c7b379471e3683d8ae6481e56250","source":{"kind":"arxiv","id":"2010.05841","version":1},"attestation_state":"computed","paper":{"title":"Bottomonium spectroscopy in the quark-gluon plasma","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Georg Wolschin","submitted_at":"2020-10-12T16:45:19Z","abstract_excerpt":"The spectroscopic properties of heavy quarkonia are substantially different in the quark-gluon plasma (QGP) that is created in relativistic heavy-ion collisions as compared to the vacuum situation that can be tested in pp collisions at the same center-of-mass energy. In this article, a series of recent works about the dissociation of the Y(nS) and chi_b(nP) states in the hot QGP is summarized. Quarkonia dissociation occurs due to (1) screening of the real quark-antiquark potential, (2) collisional damping through the imaginary part of the potential, and (3) gluon-induced dissociation. In addit"},"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":"2010.05841","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-10-12T16:45:19Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"75f9d8981f054ddf2b4e1b5e39571d690635d37d98ee7b9f9efa3667180ec21f","abstract_canon_sha256":"5438f909776535620849b504ec9aa389e8f4727ac5c206869ac687d72b217681"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:48:13.120627Z","signature_b64":"JjFhWrZqdCO18aR+qE8hGEmpon6GJ7CqILO0WUH2HqgFSBnmKJ8eKg3U2cUP5y04k0ix9Kle2wkdpwkIaOsVDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8c9e4e2a69ee5c75a5d43ce33662bfa86e64c7b379471e3683d8ae6481e56250","last_reissued_at":"2026-07-05T01:48:13.120245Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:48:13.120245Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Bottomonium spectroscopy in the quark-gluon plasma","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Georg Wolschin","submitted_at":"2020-10-12T16:45:19Z","abstract_excerpt":"The spectroscopic properties of heavy quarkonia are substantially different in the quark-gluon plasma (QGP) that is created in relativistic heavy-ion collisions as compared to the vacuum situation that can be tested in pp collisions at the same center-of-mass energy. In this article, a series of recent works about the dissociation of the Y(nS) and chi_b(nP) states in the hot QGP is summarized. Quarkonia dissociation occurs due to (1) screening of the real quark-antiquark potential, (2) collisional damping through the imaginary part of the potential, and (3) gluon-induced dissociation. In addit"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2010.05841","kind":"arxiv","version":1},"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/2010.05841/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":"2010.05841","created_at":"2026-07-05T01:48:13.120308+00:00"},{"alias_kind":"arxiv_version","alias_value":"2010.05841v1","created_at":"2026-07-05T01:48:13.120308+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2010.05841","created_at":"2026-07-05T01:48:13.120308+00:00"},{"alias_kind":"pith_short_12","alias_value":"RSPE4KTJ5ZOH","created_at":"2026-07-05T01:48:13.120308+00:00"},{"alias_kind":"pith_short_16","alias_value":"RSPE4KTJ5ZOHLJOU","created_at":"2026-07-05T01:48:13.120308+00:00"},{"alias_kind":"pith_short_8","alias_value":"RSPE4KTJ","created_at":"2026-07-05T01:48:13.120308+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2508.20995","citing_title":"Bottomonium transport in a strongly coupled quark-gluon plasma","ref_index":9,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RSPE4KTJ5ZOHLJOUHTRTMYV7VB","json":"https://pith.science/pith/RSPE4KTJ5ZOHLJOUHTRTMYV7VB.json","graph_json":"https://pith.science/api/pith-number/RSPE4KTJ5ZOHLJOUHTRTMYV7VB/graph.json","events_json":"https://pith.science/api/pith-number/RSPE4KTJ5ZOHLJOUHTRTMYV7VB/events.json","paper":"https://pith.science/paper/RSPE4KTJ"},"agent_actions":{"view_html":"https://pith.science/pith/RSPE4KTJ5ZOHLJOUHTRTMYV7VB","download_json":"https://pith.science/pith/RSPE4KTJ5ZOHLJOUHTRTMYV7VB.json","view_paper":"https://pith.science/paper/RSPE4KTJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2010.05841&json=true","fetch_graph":"https://pith.science/api/pith-number/RSPE4KTJ5ZOHLJOUHTRTMYV7VB/graph.json","fetch_events":"https://pith.science/api/pith-number/RSPE4KTJ5ZOHLJOUHTRTMYV7VB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RSPE4KTJ5ZOHLJOUHTRTMYV7VB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RSPE4KTJ5ZOHLJOUHTRTMYV7VB/action/storage_attestation","attest_author":"https://pith.science/pith/RSPE4KTJ5ZOHLJOUHTRTMYV7VB/action/author_attestation","sign_citation":"https://pith.science/pith/RSPE4KTJ5ZOHLJOUHTRTMYV7VB/action/citation_signature","submit_replication":"https://pith.science/pith/RSPE4KTJ5ZOHLJOUHTRTMYV7VB/action/replication_record"}},"created_at":"2026-07-05T01:48:13.120308+00:00","updated_at":"2026-07-05T01:48:13.120308+00:00"}