{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:QVSNZWBYZFKQVQEKBLTMUSRLOU","short_pith_number":"pith:QVSNZWBY","schema_version":"1.0","canonical_sha256":"8564dcd838c9550ac08a0ae6ca4a2b7502c8dd20cacf344ab578bad21ed79eb3","source":{"kind":"arxiv","id":"1704.00230","version":1},"attestation_state":"computed","paper":{"title":"Jet mass fluctuations and fragmentation functions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Karoly Urmossy","submitted_at":"2017-04-01T21:14:58Z","abstract_excerpt":"The effect of jet mass fluctuations on the fragmentation process is examined in the framework of a statistical hadronisation model. In this model, the fragmentation scale Q is taken to be the virtuality of the leading parton, and jet mass fluctuations are accounted for through this quantity. The scale evolution of the model is treated in the phi^3 theory with leading-order splitting function and one-loop coupling."},"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":"1704.00230","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-04-01T21:14:58Z","cross_cats_sorted":[],"title_canon_sha256":"3970cfd3399078fbbc4dba3493d8a2ddc3c71a9e36747552fe32ea3d7597f1d5","abstract_canon_sha256":"7e6fe0010ae95b1d512e3cc22082e70a521a0bddfa1dbb511a0da0275e0bd697"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:38:56.006566Z","signature_b64":"D/JCT45IycHIr0tkXpC/Nsoi8fVA00+GOygany1J1GmjLBi5hUMUM9aGVN3p7fgq/vCvQg34KeAGVkbWD0zjBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8564dcd838c9550ac08a0ae6ca4a2b7502c8dd20cacf344ab578bad21ed79eb3","last_reissued_at":"2026-05-18T00:38:56.006102Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:38:56.006102Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Jet mass fluctuations and fragmentation functions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Karoly Urmossy","submitted_at":"2017-04-01T21:14:58Z","abstract_excerpt":"The effect of jet mass fluctuations on the fragmentation process is examined in the framework of a statistical hadronisation model. In this model, the fragmentation scale Q is taken to be the virtuality of the leading parton, and jet mass fluctuations are accounted for through this quantity. The scale evolution of the model is treated in the phi^3 theory with leading-order splitting function and one-loop coupling."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.00230","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":"1704.00230","created_at":"2026-05-18T00:38:56.006166+00:00"},{"alias_kind":"arxiv_version","alias_value":"1704.00230v1","created_at":"2026-05-18T00:38:56.006166+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.00230","created_at":"2026-05-18T00:38:56.006166+00:00"},{"alias_kind":"pith_short_12","alias_value":"QVSNZWBYZFKQ","created_at":"2026-05-18T12:31:39.905425+00:00"},{"alias_kind":"pith_short_16","alias_value":"QVSNZWBYZFKQVQEK","created_at":"2026-05-18T12:31:39.905425+00:00"},{"alias_kind":"pith_short_8","alias_value":"QVSNZWBY","created_at":"2026-05-18T12:31:39.905425+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/QVSNZWBYZFKQVQEKBLTMUSRLOU","json":"https://pith.science/pith/QVSNZWBYZFKQVQEKBLTMUSRLOU.json","graph_json":"https://pith.science/api/pith-number/QVSNZWBYZFKQVQEKBLTMUSRLOU/graph.json","events_json":"https://pith.science/api/pith-number/QVSNZWBYZFKQVQEKBLTMUSRLOU/events.json","paper":"https://pith.science/paper/QVSNZWBY"},"agent_actions":{"view_html":"https://pith.science/pith/QVSNZWBYZFKQVQEKBLTMUSRLOU","download_json":"https://pith.science/pith/QVSNZWBYZFKQVQEKBLTMUSRLOU.json","view_paper":"https://pith.science/paper/QVSNZWBY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1704.00230&json=true","fetch_graph":"https://pith.science/api/pith-number/QVSNZWBYZFKQVQEKBLTMUSRLOU/graph.json","fetch_events":"https://pith.science/api/pith-number/QVSNZWBYZFKQVQEKBLTMUSRLOU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QVSNZWBYZFKQVQEKBLTMUSRLOU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QVSNZWBYZFKQVQEKBLTMUSRLOU/action/storage_attestation","attest_author":"https://pith.science/pith/QVSNZWBYZFKQVQEKBLTMUSRLOU/action/author_attestation","sign_citation":"https://pith.science/pith/QVSNZWBYZFKQVQEKBLTMUSRLOU/action/citation_signature","submit_replication":"https://pith.science/pith/QVSNZWBYZFKQVQEKBLTMUSRLOU/action/replication_record"}},"created_at":"2026-05-18T00:38:56.006166+00:00","updated_at":"2026-05-18T00:38:56.006166+00:00"}