{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:5CLJMFUZKMJR67N6LEGBG3LL6M","short_pith_number":"pith:5CLJMFUZ","schema_version":"1.0","canonical_sha256":"e89696169953131f7dbe590c136d6bf3392acb47ca158656219f8c1e8284d531","source":{"kind":"arxiv","id":"2409.04295","version":2},"attestation_state":"computed","paper":{"title":"Sensitivity of jet quenching to the initial state in heavy-ion collisions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Konrad Tywoniuk, Souvik Priyam Adhya","submitted_at":"2024-09-06T14:10:55Z","abstract_excerpt":"In heavy-ion collisions, nuclear matter is subjected to extreme conditions in a highly dynamical, rapidly evolving environment. This poses a tremendous challenge for calculating jet quenching observables. Current approaches rely on analytical results for static cases, introducing theoretical uncertainties and biases in our understanding of the pre-equilibrated medium. To address this issue, we employ resummation schemes to derive analytical rates for radiative energy loss in generic, evolving backgrounds. We investigate regimes where rare scattering and multiple scattering with the dynamical m"},"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":"2409.04295","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-09-06T14:10:55Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"867f1233d3848ecb1b4c56549654f71dd904230cad78e461490f0b06fe28a61c","abstract_canon_sha256":"3100d8bd473a394fd68a6204475040748ba8904130034cf46d15f03abf7b9433"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-29T02:04:51.277190Z","signature_b64":"osB4/x6qOsew8d255I1yVVKJwv2z+ov1NVmCEPmAzPnJfLRTXS21AMSYX16pHNTYXHOod45NFzN/irR5dkibDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e89696169953131f7dbe590c136d6bf3392acb47ca158656219f8c1e8284d531","last_reissued_at":"2026-05-29T02:04:51.274750Z","signature_status":"signed_v1","first_computed_at":"2026-05-29T02:04:51.274750Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Sensitivity of jet quenching to the initial state in heavy-ion collisions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Konrad Tywoniuk, Souvik Priyam Adhya","submitted_at":"2024-09-06T14:10:55Z","abstract_excerpt":"In heavy-ion collisions, nuclear matter is subjected to extreme conditions in a highly dynamical, rapidly evolving environment. This poses a tremendous challenge for calculating jet quenching observables. Current approaches rely on analytical results for static cases, introducing theoretical uncertainties and biases in our understanding of the pre-equilibrated medium. To address this issue, we employ resummation schemes to derive analytical rates for radiative energy loss in generic, evolving backgrounds. We investigate regimes where rare scattering and multiple scattering with the dynamical m"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2409.04295","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2409.04295/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":"2409.04295","created_at":"2026-05-29T02:04:51.274855+00:00"},{"alias_kind":"arxiv_version","alias_value":"2409.04295v2","created_at":"2026-05-29T02:04:51.274855+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2409.04295","created_at":"2026-05-29T02:04:51.274855+00:00"},{"alias_kind":"pith_short_12","alias_value":"5CLJMFUZKMJR","created_at":"2026-05-29T02:04:51.274855+00:00"},{"alias_kind":"pith_short_16","alias_value":"5CLJMFUZKMJR67N6","created_at":"2026-05-29T02:04:51.274855+00:00"},{"alias_kind":"pith_short_8","alias_value":"5CLJMFUZ","created_at":"2026-05-29T02:04:51.274855+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2605.10413","citing_title":"Light-front Hamiltonian jet evolution in the Glasma","ref_index":41,"is_internal_anchor":true},{"citing_arxiv_id":"2604.11616","citing_title":"Quantum simulating multi-particle processes in high energy nuclear physics: dijet production and color (de)coherence","ref_index":30,"is_internal_anchor":true},{"citing_arxiv_id":"2604.08520","citing_title":"Kinetic and canonical momentum broadening in the Glasma","ref_index":65,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5CLJMFUZKMJR67N6LEGBG3LL6M","json":"https://pith.science/pith/5CLJMFUZKMJR67N6LEGBG3LL6M.json","graph_json":"https://pith.science/api/pith-number/5CLJMFUZKMJR67N6LEGBG3LL6M/graph.json","events_json":"https://pith.science/api/pith-number/5CLJMFUZKMJR67N6LEGBG3LL6M/events.json","paper":"https://pith.science/paper/5CLJMFUZ"},"agent_actions":{"view_html":"https://pith.science/pith/5CLJMFUZKMJR67N6LEGBG3LL6M","download_json":"https://pith.science/pith/5CLJMFUZKMJR67N6LEGBG3LL6M.json","view_paper":"https://pith.science/paper/5CLJMFUZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2409.04295&json=true","fetch_graph":"https://pith.science/api/pith-number/5CLJMFUZKMJR67N6LEGBG3LL6M/graph.json","fetch_events":"https://pith.science/api/pith-number/5CLJMFUZKMJR67N6LEGBG3LL6M/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5CLJMFUZKMJR67N6LEGBG3LL6M/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5CLJMFUZKMJR67N6LEGBG3LL6M/action/storage_attestation","attest_author":"https://pith.science/pith/5CLJMFUZKMJR67N6LEGBG3LL6M/action/author_attestation","sign_citation":"https://pith.science/pith/5CLJMFUZKMJR67N6LEGBG3LL6M/action/citation_signature","submit_replication":"https://pith.science/pith/5CLJMFUZKMJR67N6LEGBG3LL6M/action/replication_record"}},"created_at":"2026-05-29T02:04:51.274855+00:00","updated_at":"2026-05-29T02:04:51.274855+00:00"}