{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:ORFKIICG5SXTO2OBX3YO2I6WGQ","short_pith_number":"pith:ORFKIICG","schema_version":"1.0","canonical_sha256":"744aa42046ecaf3769c1bef0ed23d6343820c007fc36ce68a1c211949b0145e2","source":{"kind":"arxiv","id":"1708.09412","version":1},"attestation_state":"computed","paper":{"title":"Ensemble-mean $\\bf p_t$ and hadron production in high-energy nuclear collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Thomas A. Trainor","submitted_at":"2017-08-30T18:13:26Z","abstract_excerpt":"A two-component (soft + hard) model (TCM) of hadron production in high-energy nuclear collisions is applied to ensemble-mean $p_t$ (denoted by $\\bar p_t$) data for $p$-$p$, $p$-Pb and Pb-Pb collisions from the relativistic heavy ion collider (RHIC) and large hadron collider (LHC). This $\\bar p_t$ TCM is directly related to a recently-published TCM for the charge-multiplicity $n_{ch}$ and collision-energy dependence of $p_t$ spectrum data from $p$-$p$ collisions. Multiplicity dependence of the $p$-$p$ spectrum hard component observed in the previous study is consistent with similar behavior for"},"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":"1708.09412","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-08-30T18:13:26Z","cross_cats_sorted":[],"title_canon_sha256":"adb6cb44b9fda18682e98702929a02e9fb0026523e60b28eee788daa019d50a6","abstract_canon_sha256":"792de278f535d9990fcbbd4a4eadc9b61090338fc2086d4e40e6fb60565ec3d1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:36:18.874921Z","signature_b64":"qxhglkyLFSg4mOIolw+Gq3Frm2cRHbMwTUyEvXEfFGs1jxFb9r9cov4d3mfk1Llan34TyY6r3yWW2EEmRtKrDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"744aa42046ecaf3769c1bef0ed23d6343820c007fc36ce68a1c211949b0145e2","last_reissued_at":"2026-05-18T00:36:18.874251Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:36:18.874251Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Ensemble-mean $\\bf p_t$ and hadron production in high-energy nuclear collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Thomas A. Trainor","submitted_at":"2017-08-30T18:13:26Z","abstract_excerpt":"A two-component (soft + hard) model (TCM) of hadron production in high-energy nuclear collisions is applied to ensemble-mean $p_t$ (denoted by $\\bar p_t$) data for $p$-$p$, $p$-Pb and Pb-Pb collisions from the relativistic heavy ion collider (RHIC) and large hadron collider (LHC). This $\\bar p_t$ TCM is directly related to a recently-published TCM for the charge-multiplicity $n_{ch}$ and collision-energy dependence of $p_t$ spectrum data from $p$-$p$ collisions. Multiplicity dependence of the $p$-$p$ spectrum hard component observed in the previous study is consistent with similar behavior for"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.09412","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":"1708.09412","created_at":"2026-05-18T00:36:18.874375+00:00"},{"alias_kind":"arxiv_version","alias_value":"1708.09412v1","created_at":"2026-05-18T00:36:18.874375+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.09412","created_at":"2026-05-18T00:36:18.874375+00:00"},{"alias_kind":"pith_short_12","alias_value":"ORFKIICG5SXT","created_at":"2026-05-18T12:31:34.259226+00:00"},{"alias_kind":"pith_short_16","alias_value":"ORFKIICG5SXTO2OB","created_at":"2026-05-18T12:31:34.259226+00:00"},{"alias_kind":"pith_short_8","alias_value":"ORFKIICG","created_at":"2026-05-18T12:31:34.259226+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2512.08003","citing_title":"Quadrupole spectra derived from 2.76 TeV Pb-Pb identified-hadron $\\bf v_2(p_t)$ data","ref_index":57,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ORFKIICG5SXTO2OBX3YO2I6WGQ","json":"https://pith.science/pith/ORFKIICG5SXTO2OBX3YO2I6WGQ.json","graph_json":"https://pith.science/api/pith-number/ORFKIICG5SXTO2OBX3YO2I6WGQ/graph.json","events_json":"https://pith.science/api/pith-number/ORFKIICG5SXTO2OBX3YO2I6WGQ/events.json","paper":"https://pith.science/paper/ORFKIICG"},"agent_actions":{"view_html":"https://pith.science/pith/ORFKIICG5SXTO2OBX3YO2I6WGQ","download_json":"https://pith.science/pith/ORFKIICG5SXTO2OBX3YO2I6WGQ.json","view_paper":"https://pith.science/paper/ORFKIICG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1708.09412&json=true","fetch_graph":"https://pith.science/api/pith-number/ORFKIICG5SXTO2OBX3YO2I6WGQ/graph.json","fetch_events":"https://pith.science/api/pith-number/ORFKIICG5SXTO2OBX3YO2I6WGQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ORFKIICG5SXTO2OBX3YO2I6WGQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ORFKIICG5SXTO2OBX3YO2I6WGQ/action/storage_attestation","attest_author":"https://pith.science/pith/ORFKIICG5SXTO2OBX3YO2I6WGQ/action/author_attestation","sign_citation":"https://pith.science/pith/ORFKIICG5SXTO2OBX3YO2I6WGQ/action/citation_signature","submit_replication":"https://pith.science/pith/ORFKIICG5SXTO2OBX3YO2I6WGQ/action/replication_record"}},"created_at":"2026-05-18T00:36:18.874375+00:00","updated_at":"2026-05-18T00:36:18.874375+00:00"}