{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:5AP5MKFC4G7D73ZK44XH5LONB6","short_pith_number":"pith:5AP5MKFC","schema_version":"1.0","canonical_sha256":"e81fd628a2e1be3fef2ae72e7eadcd0f88895b44052d1d0c682381e2914943a6","source":{"kind":"arxiv","id":"1105.2743","version":1},"attestation_state":"computed","paper":{"title":"System-size scan of dihadron azimuthal correlations in ultra-relativistic heavy ion collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"C. Zhong, G. L. Ma, J. H. Chen, S. Zhang, X. Z. Cai, Y. G. Ma, Y. H. Zhu","submitted_at":"2011-05-13T14:31:34Z","abstract_excerpt":"System-size dependence of dihadron azimuthal correlations in ultra-relativistic heavy ion collision is simulated by a multi-phase transport model. The structure of correlation functions and yields of associated particles show clear participant path-length dependences in collision systems with a partonic phase. The splitting parameter and root-mean-square width of away-side correlation functions increase with collision system size from $^{14}$N+$^{14}$N to $^{197}$Au+$^{197}$Au collisions. The double-peak structure of away-side correlation functions can only be formed in sufficient \"large\" coll"},"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":"1105.2743","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2011-05-13T14:31:34Z","cross_cats_sorted":["hep-ph","nucl-ex"],"title_canon_sha256":"573e2d44b04e45e138803e6b7a46051ac66864d39b98ded54415f98cbef1925b","abstract_canon_sha256":"f10cdaa11163ff7a94993c2a33d19de519da2969ff9ba12af4bbbc04df829d8d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:01:58.538445Z","signature_b64":"kb+8MuIP6tCgAavHV8REp66/ZGimObJBR/zCLnxFqif6uOcr8FvvNbCoI/eKV75WDQuoJCxH6hm0kiwA2RQPAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e81fd628a2e1be3fef2ae72e7eadcd0f88895b44052d1d0c682381e2914943a6","last_reissued_at":"2026-05-18T02:01:58.537784Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:01:58.537784Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"System-size scan of dihadron azimuthal correlations in ultra-relativistic heavy ion collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"C. Zhong, G. L. Ma, J. H. Chen, S. Zhang, X. Z. Cai, Y. G. Ma, Y. H. Zhu","submitted_at":"2011-05-13T14:31:34Z","abstract_excerpt":"System-size dependence of dihadron azimuthal correlations in ultra-relativistic heavy ion collision is simulated by a multi-phase transport model. The structure of correlation functions and yields of associated particles show clear participant path-length dependences in collision systems with a partonic phase. The splitting parameter and root-mean-square width of away-side correlation functions increase with collision system size from $^{14}$N+$^{14}$N to $^{197}$Au+$^{197}$Au collisions. The double-peak structure of away-side correlation functions can only be formed in sufficient \"large\" coll"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.2743","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":"1105.2743","created_at":"2026-05-18T02:01:58.537910+00:00"},{"alias_kind":"arxiv_version","alias_value":"1105.2743v1","created_at":"2026-05-18T02:01:58.537910+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.2743","created_at":"2026-05-18T02:01:58.537910+00:00"},{"alias_kind":"pith_short_12","alias_value":"5AP5MKFC4G7D","created_at":"2026-05-18T12:26:20.644004+00:00"},{"alias_kind":"pith_short_16","alias_value":"5AP5MKFC4G7D73ZK","created_at":"2026-05-18T12:26:20.644004+00:00"},{"alias_kind":"pith_short_8","alias_value":"5AP5MKFC","created_at":"2026-05-18T12:26:20.644004+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/5AP5MKFC4G7D73ZK44XH5LONB6","json":"https://pith.science/pith/5AP5MKFC4G7D73ZK44XH5LONB6.json","graph_json":"https://pith.science/api/pith-number/5AP5MKFC4G7D73ZK44XH5LONB6/graph.json","events_json":"https://pith.science/api/pith-number/5AP5MKFC4G7D73ZK44XH5LONB6/events.json","paper":"https://pith.science/paper/5AP5MKFC"},"agent_actions":{"view_html":"https://pith.science/pith/5AP5MKFC4G7D73ZK44XH5LONB6","download_json":"https://pith.science/pith/5AP5MKFC4G7D73ZK44XH5LONB6.json","view_paper":"https://pith.science/paper/5AP5MKFC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1105.2743&json=true","fetch_graph":"https://pith.science/api/pith-number/5AP5MKFC4G7D73ZK44XH5LONB6/graph.json","fetch_events":"https://pith.science/api/pith-number/5AP5MKFC4G7D73ZK44XH5LONB6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5AP5MKFC4G7D73ZK44XH5LONB6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5AP5MKFC4G7D73ZK44XH5LONB6/action/storage_attestation","attest_author":"https://pith.science/pith/5AP5MKFC4G7D73ZK44XH5LONB6/action/author_attestation","sign_citation":"https://pith.science/pith/5AP5MKFC4G7D73ZK44XH5LONB6/action/citation_signature","submit_replication":"https://pith.science/pith/5AP5MKFC4G7D73ZK44XH5LONB6/action/replication_record"}},"created_at":"2026-05-18T02:01:58.537910+00:00","updated_at":"2026-05-18T02:01:58.537910+00:00"}