{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:RBF4GD3O3NAVFCXFPDOPQP2BQJ","short_pith_number":"pith:RBF4GD3O","schema_version":"1.0","canonical_sha256":"884bc30f6edb41528ae578dcf83f41825c2ecd4b294eef1746bee67f47b979a0","source":{"kind":"arxiv","id":"2208.14419","version":2},"attestation_state":"computed","paper":{"title":"Global constraint on the jet transport coefficient from single hadron, dihadron and $\\gamma$-hadron spectra in high-energy heavy-ion collisions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Hanzhong Zhang, Man Xie, Weiyao Ke, Xin-Nian Wang","submitted_at":"2022-08-30T17:39:00Z","abstract_excerpt":"Modifications of large transverse momentum single hadron, dihadron, and $\\gamma$-hadron spectra in relativistic heavy-ion collisions are direct consequences of parton-medium interactions in the quark-gluon plasma (QGP). The interaction strength and underlying dynamics can be quantified by the jet transport coefficient $\\hat{q}$. We carry out the first global constraint on $\\hat{q}$ using a next-to-leading order pQCD parton model with higher-twist parton energy loss and combining world experimental data on single hadron, dihadron, and $\\gamma$-hadron suppression at both RHIC and LHC energies wi"},"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":"2208.14419","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-08-30T17:39:00Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"e3086ee1f63051de85b3d1c095cad4216f667692f08810898282b877cd83522a","abstract_canon_sha256":"631913d2c3d611302711b0de55160ced03ddc37b169ec860900bf4fd9a73b94e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:10:45.215540Z","signature_b64":"AGpB73+6UsakwlPi/XLPz1nZOyIJ9/UfKius9NOitc/YX66Dqco7djiJki/a+1B2cEUpooXnFRJXRRo6MVOACg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"884bc30f6edb41528ae578dcf83f41825c2ecd4b294eef1746bee67f47b979a0","last_reissued_at":"2026-07-05T07:10:45.215086Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:10:45.215086Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Global constraint on the jet transport coefficient from single hadron, dihadron and $\\gamma$-hadron spectra in high-energy heavy-ion collisions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Hanzhong Zhang, Man Xie, Weiyao Ke, Xin-Nian Wang","submitted_at":"2022-08-30T17:39:00Z","abstract_excerpt":"Modifications of large transverse momentum single hadron, dihadron, and $\\gamma$-hadron spectra in relativistic heavy-ion collisions are direct consequences of parton-medium interactions in the quark-gluon plasma (QGP). The interaction strength and underlying dynamics can be quantified by the jet transport coefficient $\\hat{q}$. We carry out the first global constraint on $\\hat{q}$ using a next-to-leading order pQCD parton model with higher-twist parton energy loss and combining world experimental data on single hadron, dihadron, and $\\gamma$-hadron suppression at both RHIC and LHC energies wi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2208.14419","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/2208.14419/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":"2208.14419","created_at":"2026-07-05T07:10:45.215138+00:00"},{"alias_kind":"arxiv_version","alias_value":"2208.14419v2","created_at":"2026-07-05T07:10:45.215138+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2208.14419","created_at":"2026-07-05T07:10:45.215138+00:00"},{"alias_kind":"pith_short_12","alias_value":"RBF4GD3O3NAV","created_at":"2026-07-05T07:10:45.215138+00:00"},{"alias_kind":"pith_short_16","alias_value":"RBF4GD3O3NAVFCXF","created_at":"2026-07-05T07:10:45.215138+00:00"},{"alias_kind":"pith_short_8","alias_value":"RBF4GD3O","created_at":"2026-07-05T07:10:45.215138+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2509.07842","citing_title":"Jet cone size dependence of single inclusive jet suppression due to jet quenching in Pb+Pb collisions at $\\sqrt{s_{\\rm NN}}=5.02$ TeV","ref_index":48,"is_internal_anchor":false},{"citing_arxiv_id":"2509.19430","citing_title":"Bayesian Constraints on Pre-Equilibrium Jet Quenching and Predictions for Oxygen Collisions","ref_index":121,"is_internal_anchor":false},{"citing_arxiv_id":"2605.02342","citing_title":"Measurement of isolated-prompt photon$-$hadron correlations in Pb$-$Pb collisions at $\\mathbf{\\sqrt{\\textit{s}_{\\rm NN}} = 5.02}$ TeV","ref_index":22,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RBF4GD3O3NAVFCXFPDOPQP2BQJ","json":"https://pith.science/pith/RBF4GD3O3NAVFCXFPDOPQP2BQJ.json","graph_json":"https://pith.science/api/pith-number/RBF4GD3O3NAVFCXFPDOPQP2BQJ/graph.json","events_json":"https://pith.science/api/pith-number/RBF4GD3O3NAVFCXFPDOPQP2BQJ/events.json","paper":"https://pith.science/paper/RBF4GD3O"},"agent_actions":{"view_html":"https://pith.science/pith/RBF4GD3O3NAVFCXFPDOPQP2BQJ","download_json":"https://pith.science/pith/RBF4GD3O3NAVFCXFPDOPQP2BQJ.json","view_paper":"https://pith.science/paper/RBF4GD3O","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2208.14419&json=true","fetch_graph":"https://pith.science/api/pith-number/RBF4GD3O3NAVFCXFPDOPQP2BQJ/graph.json","fetch_events":"https://pith.science/api/pith-number/RBF4GD3O3NAVFCXFPDOPQP2BQJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RBF4GD3O3NAVFCXFPDOPQP2BQJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RBF4GD3O3NAVFCXFPDOPQP2BQJ/action/storage_attestation","attest_author":"https://pith.science/pith/RBF4GD3O3NAVFCXFPDOPQP2BQJ/action/author_attestation","sign_citation":"https://pith.science/pith/RBF4GD3O3NAVFCXFPDOPQP2BQJ/action/citation_signature","submit_replication":"https://pith.science/pith/RBF4GD3O3NAVFCXFPDOPQP2BQJ/action/replication_record"}},"created_at":"2026-07-05T07:10:45.215138+00:00","updated_at":"2026-07-05T07:10:45.215138+00:00"}