{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:UQJ7HDOY4HKTKTLPK3RJXFWKBB","short_pith_number":"pith:UQJ7HDOY","schema_version":"1.0","canonical_sha256":"a413f38dd8e1d5354d6f56e29b96ca08729c6558b0ea6ff8d9e4959a810329c2","source":{"kind":"arxiv","id":"nucl-ex/0203015","version":1},"attestation_state":"computed","paper":{"title":"Event-by-event fluctuations in Mean $p_T$ and Mean $e_T$ in sqrt(s_NN) = 130 GeV Au+Au Collisions","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"et al, K. Adcox, PHENIX Collaboration","submitted_at":"2002-03-22T16:51:33Z","abstract_excerpt":"Distributions of event-by-event fluctuations of the mean transverse momentum and mean transverse energy near mid-rapidity have been measured in Au+Au collisions at sqrt(s_NN) = 130 GeV at RHIC. By comparing the distributions to what is expected for statistically independent particle emission, the magnitude of non-statistical fluctuations in mean transverse momentum is determined to be consistent with zero. Also, no significant non-random fluctuations in mean transverse energy are observed. By constructing a fluctuation model with two event classes that preserve the mean and variance of the sem"},"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":"nucl-ex/0203015","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-ex","submitted_at":"2002-03-22T16:51:33Z","cross_cats_sorted":[],"title_canon_sha256":"e03c5843eda4bcd7f3a40e274e32b26579744e276726c73fe5940a48b5b59350","abstract_canon_sha256":"3e8761999b17da464f117333b1081a504189c7946ee981551f17f36f38b36bc0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:32:32.261028Z","signature_b64":"801MgMNyMckjahytwPxOa1OXUXwA/4frrxrIDdQenrKw50iB9i8yq/EJdOeP0TOTTbAB+LLg7pLXUj0EgTIbAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a413f38dd8e1d5354d6f56e29b96ca08729c6558b0ea6ff8d9e4959a810329c2","last_reissued_at":"2026-07-04T15:32:32.260587Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:32:32.260587Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Event-by-event fluctuations in Mean $p_T$ and Mean $e_T$ in sqrt(s_NN) = 130 GeV Au+Au Collisions","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"et al, K. Adcox, PHENIX Collaboration","submitted_at":"2002-03-22T16:51:33Z","abstract_excerpt":"Distributions of event-by-event fluctuations of the mean transverse momentum and mean transverse energy near mid-rapidity have been measured in Au+Au collisions at sqrt(s_NN) = 130 GeV at RHIC. By comparing the distributions to what is expected for statistically independent particle emission, the magnitude of non-statistical fluctuations in mean transverse momentum is determined to be consistent with zero. Also, no significant non-random fluctuations in mean transverse energy are observed. By constructing a fluctuation model with two event classes that preserve the mean and variance of the sem"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-ex/0203015","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/nucl-ex/0203015/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":"nucl-ex/0203015","created_at":"2026-07-04T15:32:32.260648+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-ex/0203015v1","created_at":"2026-07-04T15:32:32.260648+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-ex/0203015","created_at":"2026-07-04T15:32:32.260648+00:00"},{"alias_kind":"pith_short_12","alias_value":"UQJ7HDOY4HKT","created_at":"2026-07-04T15:32:32.260648+00:00"},{"alias_kind":"pith_short_16","alias_value":"UQJ7HDOY4HKTKTLP","created_at":"2026-07-04T15:32:32.260648+00:00"},{"alias_kind":"pith_short_8","alias_value":"UQJ7HDOY","created_at":"2026-07-04T15:32:32.260648+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.09334","citing_title":"System size and energy dependence of the mean transverse momentum fluctuations at the LHC","ref_index":22,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UQJ7HDOY4HKTKTLPK3RJXFWKBB","json":"https://pith.science/pith/UQJ7HDOY4HKTKTLPK3RJXFWKBB.json","graph_json":"https://pith.science/api/pith-number/UQJ7HDOY4HKTKTLPK3RJXFWKBB/graph.json","events_json":"https://pith.science/api/pith-number/UQJ7HDOY4HKTKTLPK3RJXFWKBB/events.json","paper":"https://pith.science/paper/UQJ7HDOY"},"agent_actions":{"view_html":"https://pith.science/pith/UQJ7HDOY4HKTKTLPK3RJXFWKBB","download_json":"https://pith.science/pith/UQJ7HDOY4HKTKTLPK3RJXFWKBB.json","view_paper":"https://pith.science/paper/UQJ7HDOY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-ex/0203015&json=true","fetch_graph":"https://pith.science/api/pith-number/UQJ7HDOY4HKTKTLPK3RJXFWKBB/graph.json","fetch_events":"https://pith.science/api/pith-number/UQJ7HDOY4HKTKTLPK3RJXFWKBB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UQJ7HDOY4HKTKTLPK3RJXFWKBB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UQJ7HDOY4HKTKTLPK3RJXFWKBB/action/storage_attestation","attest_author":"https://pith.science/pith/UQJ7HDOY4HKTKTLPK3RJXFWKBB/action/author_attestation","sign_citation":"https://pith.science/pith/UQJ7HDOY4HKTKTLPK3RJXFWKBB/action/citation_signature","submit_replication":"https://pith.science/pith/UQJ7HDOY4HKTKTLPK3RJXFWKBB/action/replication_record"}},"created_at":"2026-07-04T15:32:32.260648+00:00","updated_at":"2026-07-04T15:32:32.260648+00:00"}