{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:6USTFSSO6ZU4CLOTRTIDH4VRQD","short_pith_number":"pith:6USTFSSO","schema_version":"1.0","canonical_sha256":"f52532ca4ef669c12dd38cd033f2b180d8a0e6fb41fa13c4cc8db5311c78552b","source":{"kind":"arxiv","id":"2110.02586","version":1},"attestation_state":"computed","paper":{"title":"First steps towards the quantum simulation of jet quenching","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Carlos A. Salgado, Jo\\~ao Barata","submitted_at":"2021-10-06T08:53:10Z","abstract_excerpt":"The leading order $\\alpha_s$ effect in jet quenching corresponds to the broadening of the jet's transverse momentum, due to the multiple interactions with the underlying medium. A complete understanding of momentum broadening is critical for the success of jet quenching phenomenology.\n  In this talk, we introduce a strategy to quantum simulate single particle momentum broadening in a QCD background medium. We argue that it is, in principle, possible to extract the jet quenching parameter $\\hat{q}$ from such an algorithm. More importantly, this corresponds to the first step towards simulating f"},"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":"2110.02586","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2021-10-06T08:53:10Z","cross_cats_sorted":[],"title_canon_sha256":"662896ce1ec3c05830b1c52ade19114a6bad502a5061665f16f2ac8296fd8bfc","abstract_canon_sha256":"37b8b5b0a0e19f582dc08fac573e6b618dc3c8565650faa618bd26df249e960e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:20:27.981622Z","signature_b64":"4UCB728MOIizaYfhCKrzcMeQsLP+5dFojJrdfyy8rox4fEUpt0G/G/gWBXejquyB9AX1UgqFQueciS3VFjiTDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f52532ca4ef669c12dd38cd033f2b180d8a0e6fb41fa13c4cc8db5311c78552b","last_reissued_at":"2026-07-05T03:20:27.981167Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:20:27.981167Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"First steps towards the quantum simulation of jet quenching","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Carlos A. Salgado, Jo\\~ao Barata","submitted_at":"2021-10-06T08:53:10Z","abstract_excerpt":"The leading order $\\alpha_s$ effect in jet quenching corresponds to the broadening of the jet's transverse momentum, due to the multiple interactions with the underlying medium. A complete understanding of momentum broadening is critical for the success of jet quenching phenomenology.\n  In this talk, we introduce a strategy to quantum simulate single particle momentum broadening in a QCD background medium. We argue that it is, in principle, possible to extract the jet quenching parameter $\\hat{q}$ from such an algorithm. More importantly, this corresponds to the first step towards simulating f"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2110.02586","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/2110.02586/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":"2110.02586","created_at":"2026-07-05T03:20:27.981220+00:00"},{"alias_kind":"arxiv_version","alias_value":"2110.02586v1","created_at":"2026-07-05T03:20:27.981220+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2110.02586","created_at":"2026-07-05T03:20:27.981220+00:00"},{"alias_kind":"pith_short_12","alias_value":"6USTFSSO6ZU4","created_at":"2026-07-05T03:20:27.981220+00:00"},{"alias_kind":"pith_short_16","alias_value":"6USTFSSO6ZU4CLOT","created_at":"2026-07-05T03:20:27.981220+00:00"},{"alias_kind":"pith_short_8","alias_value":"6USTFSSO","created_at":"2026-07-05T03:20:27.981220+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2608.06754","citing_title":"Quantum simulation of bottomonium dynamics in the quark-gluon plasma via the Lindblad equation","ref_index":36,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6USTFSSO6ZU4CLOTRTIDH4VRQD","json":"https://pith.science/pith/6USTFSSO6ZU4CLOTRTIDH4VRQD.json","graph_json":"https://pith.science/api/pith-number/6USTFSSO6ZU4CLOTRTIDH4VRQD/graph.json","events_json":"https://pith.science/api/pith-number/6USTFSSO6ZU4CLOTRTIDH4VRQD/events.json","paper":"https://pith.science/paper/6USTFSSO"},"agent_actions":{"view_html":"https://pith.science/pith/6USTFSSO6ZU4CLOTRTIDH4VRQD","download_json":"https://pith.science/pith/6USTFSSO6ZU4CLOTRTIDH4VRQD.json","view_paper":"https://pith.science/paper/6USTFSSO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2110.02586&json=true","fetch_graph":"https://pith.science/api/pith-number/6USTFSSO6ZU4CLOTRTIDH4VRQD/graph.json","fetch_events":"https://pith.science/api/pith-number/6USTFSSO6ZU4CLOTRTIDH4VRQD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6USTFSSO6ZU4CLOTRTIDH4VRQD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6USTFSSO6ZU4CLOTRTIDH4VRQD/action/storage_attestation","attest_author":"https://pith.science/pith/6USTFSSO6ZU4CLOTRTIDH4VRQD/action/author_attestation","sign_citation":"https://pith.science/pith/6USTFSSO6ZU4CLOTRTIDH4VRQD/action/citation_signature","submit_replication":"https://pith.science/pith/6USTFSSO6ZU4CLOTRTIDH4VRQD/action/replication_record"}},"created_at":"2026-07-05T03:20:27.981220+00:00","updated_at":"2026-07-05T03:20:27.981220+00:00"}