{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:LR7QOYBGAB4F75NZNTH7HSYGLO","short_pith_number":"pith:LR7QOYBG","schema_version":"1.0","canonical_sha256":"5c7f07602600785ff5b96ccff3cb065b9956a77875ff9c38ea7502f1a25cb5f8","source":{"kind":"arxiv","id":"hep-ph/9610420","version":1},"attestation_state":"computed","paper":{"title":"Determining the existence and nature of the quark-gluon plasma by Upsilon suppression at the LHC","license":"","headline":"","cross_cats":["hep-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"J.F. Gunion (U.C. Davis), R. Vogt (LBNL, U.C. Davis)","submitted_at":"1996-10-19T22:19:55Z","abstract_excerpt":"Minijet production in $\\sqrt{s} = 5.5$ TeV Pb+Pb collisions at the LHC is expected to produce a gluon-dominated plasma with large initial temperatures and energy densities. We discuss the implications of the high initial temperatures on the screening mass and on the relative suppression of members of the $\\Upsilon$ family. We demonstrate that $p_T$-dependence of the $\\Upsilon'/\\Upsilon$ ratio is only expected if a quark-gluon plasma with significant energy density is present, and that the precise dependence of this ratio will strongly constrain the QGP models. We also propose that the $p_T$ sp"},"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":"hep-ph/9610420","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1996-10-19T22:19:55Z","cross_cats_sorted":["hep-ex","nucl-th"],"title_canon_sha256":"b77555363571ed6748eac43862271f00b1970eb5f2b3e86ec50153a956dcd402","abstract_canon_sha256":"db829afbef969f2191e9a77ab1a08686cbfb622314c9aefb9fd67cefa3ab4413"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:38:58.875199Z","signature_b64":"CjuqhM9PxeV8zfd4cFiyJFXeOb7+DspHuXW+eyDToktkgxLG/biG+QNM5vc2EM6PYI/Qn+g7W7YUVL5ASX35BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5c7f07602600785ff5b96ccff3cb065b9956a77875ff9c38ea7502f1a25cb5f8","last_reissued_at":"2026-05-18T01:38:58.874479Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:38:58.874479Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Determining the existence and nature of the quark-gluon plasma by Upsilon suppression at the LHC","license":"","headline":"","cross_cats":["hep-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"J.F. Gunion (U.C. Davis), R. Vogt (LBNL, U.C. Davis)","submitted_at":"1996-10-19T22:19:55Z","abstract_excerpt":"Minijet production in $\\sqrt{s} = 5.5$ TeV Pb+Pb collisions at the LHC is expected to produce a gluon-dominated plasma with large initial temperatures and energy densities. We discuss the implications of the high initial temperatures on the screening mass and on the relative suppression of members of the $\\Upsilon$ family. We demonstrate that $p_T$-dependence of the $\\Upsilon'/\\Upsilon$ ratio is only expected if a quark-gluon plasma with significant energy density is present, and that the precise dependence of this ratio will strongly constrain the QGP models. We also propose that the $p_T$ sp"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9610420","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":""},"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":"hep-ph/9610420","created_at":"2026-05-18T01:38:58.874596+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9610420v1","created_at":"2026-05-18T01:38:58.874596+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9610420","created_at":"2026-05-18T01:38:58.874596+00:00"},{"alias_kind":"pith_short_12","alias_value":"LR7QOYBGAB4F","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_16","alias_value":"LR7QOYBGAB4F75NZ","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_8","alias_value":"LR7QOYBG","created_at":"2026-05-18T12:25:48.327863+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"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":33,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LR7QOYBGAB4F75NZNTH7HSYGLO","json":"https://pith.science/pith/LR7QOYBGAB4F75NZNTH7HSYGLO.json","graph_json":"https://pith.science/api/pith-number/LR7QOYBGAB4F75NZNTH7HSYGLO/graph.json","events_json":"https://pith.science/api/pith-number/LR7QOYBGAB4F75NZNTH7HSYGLO/events.json","paper":"https://pith.science/paper/LR7QOYBG"},"agent_actions":{"view_html":"https://pith.science/pith/LR7QOYBGAB4F75NZNTH7HSYGLO","download_json":"https://pith.science/pith/LR7QOYBGAB4F75NZNTH7HSYGLO.json","view_paper":"https://pith.science/paper/LR7QOYBG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9610420&json=true","fetch_graph":"https://pith.science/api/pith-number/LR7QOYBGAB4F75NZNTH7HSYGLO/graph.json","fetch_events":"https://pith.science/api/pith-number/LR7QOYBGAB4F75NZNTH7HSYGLO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LR7QOYBGAB4F75NZNTH7HSYGLO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LR7QOYBGAB4F75NZNTH7HSYGLO/action/storage_attestation","attest_author":"https://pith.science/pith/LR7QOYBGAB4F75NZNTH7HSYGLO/action/author_attestation","sign_citation":"https://pith.science/pith/LR7QOYBGAB4F75NZNTH7HSYGLO/action/citation_signature","submit_replication":"https://pith.science/pith/LR7QOYBGAB4F75NZNTH7HSYGLO/action/replication_record"}},"created_at":"2026-05-18T01:38:58.874596+00:00","updated_at":"2026-05-18T01:38:58.874596+00:00"}