{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:6VH7RQ4E3SEV4IOF3A56RF5NM3","short_pith_number":"pith:6VH7RQ4E","schema_version":"1.0","canonical_sha256":"f54ff8c384dc895e21c5d83be897ad66d21814bfc1c76d8d721b6b112a1a8893","source":{"kind":"arxiv","id":"2407.19966","version":1},"attestation_state":"computed","paper":{"title":"QCD jets in a hot and dense medium: a study of shower formation time and collision kernels","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Charles Gale, Rouzbeh Modarresi-Yazdi, Sangyong Jeon, Shuzhe Shi","submitted_at":"2024-07-29T12:58:00Z","abstract_excerpt":"With the use of MARTINI, a model which considers evolving QCD jets against a fluid dynamical background, it is shown that the introduction of formation time to the parton shower after the initial hard scattering is essential for a simultaneous description of charged hadron and jet $R_{AA}$. This inclusion also improves jet shape ratio at small angle and jet fragmentation function ratios of leading charged hadrons. The MARTINI framework is then aimed at a study of the leading order, next-to-leading-order, and non perturbative collision kernels. Sizable differences in the modification of jet sub"},"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":"2407.19966","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-07-29T12:58:00Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"c6429a8f66b4f52b4bad14f93f606370806db4bc2a112d16c7f55a9a5f982cb8","abstract_canon_sha256":"0aa67a46403a4603fc0064b62f50e5df54a2036b11ff433637a033c0a037341e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:49:47.000190Z","signature_b64":"rfkLaqYd42TpE+wdDbzsSnn2ls4j57sRgb/zesad4X5gwbACulniUdD/J0A+zaRpblogF+ObBYRCzvEy7xWnBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f54ff8c384dc895e21c5d83be897ad66d21814bfc1c76d8d721b6b112a1a8893","last_reissued_at":"2026-07-05T08:49:46.999786Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:49:46.999786Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"QCD jets in a hot and dense medium: a study of shower formation time and collision kernels","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Charles Gale, Rouzbeh Modarresi-Yazdi, Sangyong Jeon, Shuzhe Shi","submitted_at":"2024-07-29T12:58:00Z","abstract_excerpt":"With the use of MARTINI, a model which considers evolving QCD jets against a fluid dynamical background, it is shown that the introduction of formation time to the parton shower after the initial hard scattering is essential for a simultaneous description of charged hadron and jet $R_{AA}$. This inclusion also improves jet shape ratio at small angle and jet fragmentation function ratios of leading charged hadrons. The MARTINI framework is then aimed at a study of the leading order, next-to-leading-order, and non perturbative collision kernels. Sizable differences in the modification of jet sub"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2407.19966","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/2407.19966/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":"2407.19966","created_at":"2026-07-05T08:49:46.999840+00:00"},{"alias_kind":"arxiv_version","alias_value":"2407.19966v1","created_at":"2026-07-05T08:49:46.999840+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2407.19966","created_at":"2026-07-05T08:49:46.999840+00:00"},{"alias_kind":"pith_short_12","alias_value":"6VH7RQ4E3SEV","created_at":"2026-07-05T08:49:46.999840+00:00"},{"alias_kind":"pith_short_16","alias_value":"6VH7RQ4E3SEV4IOF","created_at":"2026-07-05T08:49:46.999840+00:00"},{"alias_kind":"pith_short_8","alias_value":"6VH7RQ4E","created_at":"2026-07-05T08:49:46.999840+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2509.10743","citing_title":"Glauber quark and gluon contributions to quark energy loss at next-to-leading order and next-to-leading twist","ref_index":54,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6VH7RQ4E3SEV4IOF3A56RF5NM3","json":"https://pith.science/pith/6VH7RQ4E3SEV4IOF3A56RF5NM3.json","graph_json":"https://pith.science/api/pith-number/6VH7RQ4E3SEV4IOF3A56RF5NM3/graph.json","events_json":"https://pith.science/api/pith-number/6VH7RQ4E3SEV4IOF3A56RF5NM3/events.json","paper":"https://pith.science/paper/6VH7RQ4E"},"agent_actions":{"view_html":"https://pith.science/pith/6VH7RQ4E3SEV4IOF3A56RF5NM3","download_json":"https://pith.science/pith/6VH7RQ4E3SEV4IOF3A56RF5NM3.json","view_paper":"https://pith.science/paper/6VH7RQ4E","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2407.19966&json=true","fetch_graph":"https://pith.science/api/pith-number/6VH7RQ4E3SEV4IOF3A56RF5NM3/graph.json","fetch_events":"https://pith.science/api/pith-number/6VH7RQ4E3SEV4IOF3A56RF5NM3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6VH7RQ4E3SEV4IOF3A56RF5NM3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6VH7RQ4E3SEV4IOF3A56RF5NM3/action/storage_attestation","attest_author":"https://pith.science/pith/6VH7RQ4E3SEV4IOF3A56RF5NM3/action/author_attestation","sign_citation":"https://pith.science/pith/6VH7RQ4E3SEV4IOF3A56RF5NM3/action/citation_signature","submit_replication":"https://pith.science/pith/6VH7RQ4E3SEV4IOF3A56RF5NM3/action/replication_record"}},"created_at":"2026-07-05T08:49:46.999840+00:00","updated_at":"2026-07-05T08:49:46.999840+00:00"}