{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:NIBOTW3PS3SRIC5EB6EJCP2MVC","short_pith_number":"pith:NIBOTW3P","schema_version":"1.0","canonical_sha256":"6a02e9db6f96e5140ba40f88913f4ca8b0cb38455c69fffdc1f13972de27a1c3","source":{"kind":"arxiv","id":"2506.10702","version":4},"attestation_state":"computed","paper":{"title":"Extraction of Effective Parameters from Transverse Momentum Spectra of Heavy Quarkonia in Proton-Proton Collisions at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Fu-Hu Liu, Hailong Zhu, Khusniddin K. Olimov, Peng-Cheng Zhang","submitted_at":"2025-06-12T13:51:32Z","abstract_excerpt":"The effective string tension ($\\kappa$) in the Schwinger mechanism and the effective temperature ($T$) in Bose-Einstein statistics are extracted from the transverse momentum ($p_T$) spectra of heavy quarkonia produced in proton-proton (p+p) collisions at the Large Hadron Collider (LHC). Here, $T$ derived from the heavy quarkonium $p_T$ spectra also serves as the initial effective temperature (effective temperature at the initial stage) of small collision systems. This is because, despite the absence of quark-gluon plasma (QGP) formation during the collisions, which leaves $T$ largely unaffecte"},"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":"2506.10702","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-06-12T13:51:32Z","cross_cats_sorted":["hep-ex","nucl-ex","nucl-th"],"title_canon_sha256":"69dec95708eeefd5705811c23d407f8418e7e903212644e47565de8091281785","abstract_canon_sha256":"569773bc84c1bce3f01175f00a20235fd1aa4e998cb48c5f0155f7c4820d4a2e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-21T01:04:14.594572Z","signature_b64":"duraNW0pvAwFzo5FSEKYlCNa2bI+i2OF46fXlDSuywJlv2CZ1OJ7tvESSzB8ZwiQ3WT5Lj2C8oQhQwAMFxhYBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6a02e9db6f96e5140ba40f88913f4ca8b0cb38455c69fffdc1f13972de27a1c3","last_reissued_at":"2026-05-21T01:04:14.593702Z","signature_status":"signed_v1","first_computed_at":"2026-05-21T01:04:14.593702Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Extraction of Effective Parameters from Transverse Momentum Spectra of Heavy Quarkonia in Proton-Proton Collisions at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Fu-Hu Liu, Hailong Zhu, Khusniddin K. Olimov, Peng-Cheng Zhang","submitted_at":"2025-06-12T13:51:32Z","abstract_excerpt":"The effective string tension ($\\kappa$) in the Schwinger mechanism and the effective temperature ($T$) in Bose-Einstein statistics are extracted from the transverse momentum ($p_T$) spectra of heavy quarkonia produced in proton-proton (p+p) collisions at the Large Hadron Collider (LHC). Here, $T$ derived from the heavy quarkonium $p_T$ spectra also serves as the initial effective temperature (effective temperature at the initial stage) of small collision systems. This is because, despite the absence of quark-gluon plasma (QGP) formation during the collisions, which leaves $T$ largely unaffecte"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.10702","kind":"arxiv","version":4},"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/2506.10702/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":"2506.10702","created_at":"2026-05-21T01:04:14.593830+00:00"},{"alias_kind":"arxiv_version","alias_value":"2506.10702v4","created_at":"2026-05-21T01:04:14.593830+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.10702","created_at":"2026-05-21T01:04:14.593830+00:00"},{"alias_kind":"pith_short_12","alias_value":"NIBOTW3PS3SR","created_at":"2026-05-21T01:04:14.593830+00:00"},{"alias_kind":"pith_short_16","alias_value":"NIBOTW3PS3SRIC5E","created_at":"2026-05-21T01:04:14.593830+00:00"},{"alias_kind":"pith_short_8","alias_value":"NIBOTW3P","created_at":"2026-05-21T01:04:14.593830+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NIBOTW3PS3SRIC5EB6EJCP2MVC","json":"https://pith.science/pith/NIBOTW3PS3SRIC5EB6EJCP2MVC.json","graph_json":"https://pith.science/api/pith-number/NIBOTW3PS3SRIC5EB6EJCP2MVC/graph.json","events_json":"https://pith.science/api/pith-number/NIBOTW3PS3SRIC5EB6EJCP2MVC/events.json","paper":"https://pith.science/paper/NIBOTW3P"},"agent_actions":{"view_html":"https://pith.science/pith/NIBOTW3PS3SRIC5EB6EJCP2MVC","download_json":"https://pith.science/pith/NIBOTW3PS3SRIC5EB6EJCP2MVC.json","view_paper":"https://pith.science/paper/NIBOTW3P","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2506.10702&json=true","fetch_graph":"https://pith.science/api/pith-number/NIBOTW3PS3SRIC5EB6EJCP2MVC/graph.json","fetch_events":"https://pith.science/api/pith-number/NIBOTW3PS3SRIC5EB6EJCP2MVC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NIBOTW3PS3SRIC5EB6EJCP2MVC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NIBOTW3PS3SRIC5EB6EJCP2MVC/action/storage_attestation","attest_author":"https://pith.science/pith/NIBOTW3PS3SRIC5EB6EJCP2MVC/action/author_attestation","sign_citation":"https://pith.science/pith/NIBOTW3PS3SRIC5EB6EJCP2MVC/action/citation_signature","submit_replication":"https://pith.science/pith/NIBOTW3PS3SRIC5EB6EJCP2MVC/action/replication_record"}},"created_at":"2026-05-21T01:04:14.593830+00:00","updated_at":"2026-05-21T01:04:14.593830+00:00"}