{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:K2J3F2SOQK4TEFGPDIJ6EZNKGI","short_pith_number":"pith:K2J3F2SO","schema_version":"1.0","canonical_sha256":"5693b2ea4e82b93214cf1a13e265aa32038d1432957824879bade26ed52baae5","source":{"kind":"arxiv","id":"2406.17592","version":1},"attestation_state":"computed","paper":{"title":"MC-EKRT: Monte Carlo event generator with saturated minijet production for initializing 3+1 D fluid dynamics in high energy nuclear collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Harri Niemi, Henry Hirvonen, Jussi Auvinen, Kari J. Eskola, Mikko Kuha, Yuuka Kanakubo","submitted_at":"2024-06-25T14:33:56Z","abstract_excerpt":"We present a novel Monte-Carlo implementation of the EKRT model, MC-EKRT, for computing partonic initial states in high-energy nuclear collisions. Our new MC-EKRT event generator is based on collinearly factorized, dynamically fluctuating pQCD minijet production, supplemented with a saturation conjecture that controls the low-$p_T$ particle production. Previously, the EKRT model has been very successful in describing low-$p_T$ observables at mid-rapidity in heavy-ion collisions at the LHC and RHIC energies. As novel features, our new MC implementation gives a full 3-dimensional initial state e"},"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":"2406.17592","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-06-25T14:33:56Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"87a2f3d041b15fc8dfbc85ec987df748cec9dfed4caf923e498d7c4396ae2161","abstract_canon_sha256":"28561ba52fd49b5983c443767537dd33f51887ded2c72e672c80aebbc10b4f09"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:36:37.456964Z","signature_b64":"82F/PpU8j07bUIXtuGnwehA5tD+zDu3r6thA3u0f5WIqFS6Ykuq/q1U3iBD1asbzFCe8GQGO4OduxGOuNGWEDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5693b2ea4e82b93214cf1a13e265aa32038d1432957824879bade26ed52baae5","last_reissued_at":"2026-07-05T08:36:37.456470Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:36:37.456470Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"MC-EKRT: Monte Carlo event generator with saturated minijet production for initializing 3+1 D fluid dynamics in high energy nuclear collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Harri Niemi, Henry Hirvonen, Jussi Auvinen, Kari J. Eskola, Mikko Kuha, Yuuka Kanakubo","submitted_at":"2024-06-25T14:33:56Z","abstract_excerpt":"We present a novel Monte-Carlo implementation of the EKRT model, MC-EKRT, for computing partonic initial states in high-energy nuclear collisions. Our new MC-EKRT event generator is based on collinearly factorized, dynamically fluctuating pQCD minijet production, supplemented with a saturation conjecture that controls the low-$p_T$ particle production. Previously, the EKRT model has been very successful in describing low-$p_T$ observables at mid-rapidity in heavy-ion collisions at the LHC and RHIC energies. As novel features, our new MC implementation gives a full 3-dimensional initial state e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2406.17592","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/2406.17592/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":"2406.17592","created_at":"2026-07-05T08:36:37.456532+00:00"},{"alias_kind":"arxiv_version","alias_value":"2406.17592v1","created_at":"2026-07-05T08:36:37.456532+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2406.17592","created_at":"2026-07-05T08:36:37.456532+00:00"},{"alias_kind":"pith_short_12","alias_value":"K2J3F2SOQK4T","created_at":"2026-07-05T08:36:37.456532+00:00"},{"alias_kind":"pith_short_16","alias_value":"K2J3F2SOQK4TEFGP","created_at":"2026-07-05T08:36:37.456532+00:00"},{"alias_kind":"pith_short_8","alias_value":"K2J3F2SO","created_at":"2026-07-05T08:36:37.456532+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2512.08007","citing_title":"(3+1)D event-by-event pre-equilibrium dynamics in heavy-ion collisions","ref_index":17,"is_internal_anchor":false},{"citing_arxiv_id":"2605.16914","citing_title":"3D Initial-State Dynamics across scales: A Comparative Study of saturation and string-based descriptions","ref_index":22,"is_internal_anchor":false},{"citing_arxiv_id":"2604.15737","citing_title":"Bayesian inference constraints on jet quenching across centrality, beam energy, and observable classes in LHC heavy-ion collisions","ref_index":124,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/K2J3F2SOQK4TEFGPDIJ6EZNKGI","json":"https://pith.science/pith/K2J3F2SOQK4TEFGPDIJ6EZNKGI.json","graph_json":"https://pith.science/api/pith-number/K2J3F2SOQK4TEFGPDIJ6EZNKGI/graph.json","events_json":"https://pith.science/api/pith-number/K2J3F2SOQK4TEFGPDIJ6EZNKGI/events.json","paper":"https://pith.science/paper/K2J3F2SO"},"agent_actions":{"view_html":"https://pith.science/pith/K2J3F2SOQK4TEFGPDIJ6EZNKGI","download_json":"https://pith.science/pith/K2J3F2SOQK4TEFGPDIJ6EZNKGI.json","view_paper":"https://pith.science/paper/K2J3F2SO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2406.17592&json=true","fetch_graph":"https://pith.science/api/pith-number/K2J3F2SOQK4TEFGPDIJ6EZNKGI/graph.json","fetch_events":"https://pith.science/api/pith-number/K2J3F2SOQK4TEFGPDIJ6EZNKGI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/K2J3F2SOQK4TEFGPDIJ6EZNKGI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/K2J3F2SOQK4TEFGPDIJ6EZNKGI/action/storage_attestation","attest_author":"https://pith.science/pith/K2J3F2SOQK4TEFGPDIJ6EZNKGI/action/author_attestation","sign_citation":"https://pith.science/pith/K2J3F2SOQK4TEFGPDIJ6EZNKGI/action/citation_signature","submit_replication":"https://pith.science/pith/K2J3F2SOQK4TEFGPDIJ6EZNKGI/action/replication_record"}},"created_at":"2026-07-05T08:36:37.456532+00:00","updated_at":"2026-07-05T08:36:37.456532+00:00"}