{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:NPYYKUKB76PT7GCV5LPLLVI6LA","short_pith_number":"pith:NPYYKUKB","schema_version":"1.0","canonical_sha256":"6bf1855141ff9f3f9855eadeb5d51e5814de81b3767535260ff5a9c2b52b0c1f","source":{"kind":"arxiv","id":"1201.6382","version":2},"attestation_state":"computed","paper":{"title":"KNO scaling of fluctuations in pp and pA, and eccentricities in 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":"Adrian Dumitru, Yasushi Nara","submitted_at":"2012-01-30T21:33:05Z","abstract_excerpt":"Multiplicity fluctuations at midrapidity in p+p collisions at high energies are described by a negative binomial distribution and exhibit approximate Koba-Nielsen-Olesen (KNO) scaling. We find that these KNO fluctuations are important also for reproducing the multiplicity distribution in d+Au collisions observed at RHIC, adding to the Glauber fluctuations of the number of binary collisions or participants. We predict that the multiplicity distribution in p+Pb collisions at the LHC also deviates little from the KNO scaling function. Finally, we analyze various moments of the eccentricity of the"},"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":"1201.6382","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-01-30T21:33:05Z","cross_cats_sorted":["hep-ph","nucl-ex"],"title_canon_sha256":"854b36ba94c8b322d350ab14b694ab95f3672cbb865b09b6f305fac6e0df6b07","abstract_canon_sha256":"ea5ea68725408ba830785292e0a601ccaecec5b4238a6a96eedc142237b59987"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:57:26.566302Z","signature_b64":"avexrR+YvXOIHkkMUHEUIS/TFFA3DttVawkVzf5yuFEsq6u/SaPAx6e0aFqSLdZcdNdh26y7iobM9DBJBMCOCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6bf1855141ff9f3f9855eadeb5d51e5814de81b3767535260ff5a9c2b52b0c1f","last_reissued_at":"2026-05-18T03:57:26.565401Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:57:26.565401Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"KNO scaling of fluctuations in pp and pA, and eccentricities in 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":"Adrian Dumitru, Yasushi Nara","submitted_at":"2012-01-30T21:33:05Z","abstract_excerpt":"Multiplicity fluctuations at midrapidity in p+p collisions at high energies are described by a negative binomial distribution and exhibit approximate Koba-Nielsen-Olesen (KNO) scaling. We find that these KNO fluctuations are important also for reproducing the multiplicity distribution in d+Au collisions observed at RHIC, adding to the Glauber fluctuations of the number of binary collisions or participants. We predict that the multiplicity distribution in p+Pb collisions at the LHC also deviates little from the KNO scaling function. Finally, we analyze various moments of the eccentricity of the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.6382","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":""},"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":"1201.6382","created_at":"2026-05-18T03:57:26.565507+00:00"},{"alias_kind":"arxiv_version","alias_value":"1201.6382v2","created_at":"2026-05-18T03:57:26.565507+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.6382","created_at":"2026-05-18T03:57:26.565507+00:00"},{"alias_kind":"pith_short_12","alias_value":"NPYYKUKB76PT","created_at":"2026-05-18T12:27:16.716162+00:00"},{"alias_kind":"pith_short_16","alias_value":"NPYYKUKB76PT7GCV","created_at":"2026-05-18T12:27:16.716162+00:00"},{"alias_kind":"pith_short_8","alias_value":"NPYYKUKB","created_at":"2026-05-18T12:27:16.716162+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.15494","citing_title":"Forward hadron production in pp collisions at LHC energies from an event generator based on the color glass condensate framework","ref_index":65,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NPYYKUKB76PT7GCV5LPLLVI6LA","json":"https://pith.science/pith/NPYYKUKB76PT7GCV5LPLLVI6LA.json","graph_json":"https://pith.science/api/pith-number/NPYYKUKB76PT7GCV5LPLLVI6LA/graph.json","events_json":"https://pith.science/api/pith-number/NPYYKUKB76PT7GCV5LPLLVI6LA/events.json","paper":"https://pith.science/paper/NPYYKUKB"},"agent_actions":{"view_html":"https://pith.science/pith/NPYYKUKB76PT7GCV5LPLLVI6LA","download_json":"https://pith.science/pith/NPYYKUKB76PT7GCV5LPLLVI6LA.json","view_paper":"https://pith.science/paper/NPYYKUKB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1201.6382&json=true","fetch_graph":"https://pith.science/api/pith-number/NPYYKUKB76PT7GCV5LPLLVI6LA/graph.json","fetch_events":"https://pith.science/api/pith-number/NPYYKUKB76PT7GCV5LPLLVI6LA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NPYYKUKB76PT7GCV5LPLLVI6LA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NPYYKUKB76PT7GCV5LPLLVI6LA/action/storage_attestation","attest_author":"https://pith.science/pith/NPYYKUKB76PT7GCV5LPLLVI6LA/action/author_attestation","sign_citation":"https://pith.science/pith/NPYYKUKB76PT7GCV5LPLLVI6LA/action/citation_signature","submit_replication":"https://pith.science/pith/NPYYKUKB76PT7GCV5LPLLVI6LA/action/replication_record"}},"created_at":"2026-05-18T03:57:26.565507+00:00","updated_at":"2026-05-18T03:57:26.565507+00:00"}