{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:P67FHJ5DWMWTCIPKCDN7GHP7VM","short_pith_number":"pith:P67FHJ5D","schema_version":"1.0","canonical_sha256":"7fbe53a7a3b32d3121ea10dbf31dffab22f6375a36a0d1094320c806f012905c","source":{"kind":"arxiv","id":"2105.01679","version":4},"attestation_state":"computed","paper":{"title":"Non-perturbative determination of collisional broadening and medium induced radiation in QCD plasmas","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"Guy D. Moore, Ismail Soudi, Niels Schlusser, Soeren Schlichting","submitted_at":"2021-05-04T18:01:02Z","abstract_excerpt":"We supply recently obtained results from lattice EQCD with the correct UV limit to construct the collisional broadening kernel $C(b_\\perp)$ in a QCD plasma. We discuss the limiting behavior of $C(b_\\perp)$ at small and large impact parameters $b_\\perp$, and illustrate how the results can be used to compute medium-induced radiation rates."},"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":"2105.01679","kind":"arxiv","version":4},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2021-05-04T18:01:02Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"beaf3293b1c52fef449179d59bac4fc816694c4ef020df8617511b3f6410da1d","abstract_canon_sha256":"7b7dc418fd3a3f8700d5ca349349f1540e97ad2619a256f30e7589baf9c78e8c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:26:01.467841Z","signature_b64":"BbBYIGRBkeeT/3monJl1oONb6PLx4UV4kYf1Xvy92vIbSlrW7BHHin/S9xnUJE6cEdph1b8rYnhOi+FWNTvSDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7fbe53a7a3b32d3121ea10dbf31dffab22f6375a36a0d1094320c806f012905c","last_reissued_at":"2026-07-05T05:26:01.467348Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:26:01.467348Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-perturbative determination of collisional broadening and medium induced radiation in QCD plasmas","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"Guy D. Moore, Ismail Soudi, Niels Schlusser, Soeren Schlichting","submitted_at":"2021-05-04T18:01:02Z","abstract_excerpt":"We supply recently obtained results from lattice EQCD with the correct UV limit to construct the collisional broadening kernel $C(b_\\perp)$ in a QCD plasma. We discuss the limiting behavior of $C(b_\\perp)$ at small and large impact parameters $b_\\perp$, and illustrate how the results can be used to compute medium-induced radiation rates."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2105.01679","kind":"arxiv","version":4},"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/2105.01679/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":"2105.01679","created_at":"2026-07-05T05:26:01.467411+00:00"},{"alias_kind":"arxiv_version","alias_value":"2105.01679v4","created_at":"2026-07-05T05:26:01.467411+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2105.01679","created_at":"2026-07-05T05:26:01.467411+00:00"},{"alias_kind":"pith_short_12","alias_value":"P67FHJ5DWMWT","created_at":"2026-07-05T05:26:01.467411+00:00"},{"alias_kind":"pith_short_16","alias_value":"P67FHJ5DWMWTCIPK","created_at":"2026-07-05T05:26:01.467411+00:00"},{"alias_kind":"pith_short_8","alias_value":"P67FHJ5D","created_at":"2026-07-05T05:26:01.467411+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.07744","citing_title":"Open quantum system approach to the transverse momentum broadening of a colour dipole","ref_index":106,"is_internal_anchor":false},{"citing_arxiv_id":"2607.00629","citing_title":"Gluon radiation from a QCD antenna with realistic parton-medium interactions","ref_index":72,"is_internal_anchor":false},{"citing_arxiv_id":"2603.27846","citing_title":"Full energy fraction and angular dependence of medium-induced splittings in the large-$N_c$ limit","ref_index":73,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/P67FHJ5DWMWTCIPKCDN7GHP7VM","json":"https://pith.science/pith/P67FHJ5DWMWTCIPKCDN7GHP7VM.json","graph_json":"https://pith.science/api/pith-number/P67FHJ5DWMWTCIPKCDN7GHP7VM/graph.json","events_json":"https://pith.science/api/pith-number/P67FHJ5DWMWTCIPKCDN7GHP7VM/events.json","paper":"https://pith.science/paper/P67FHJ5D"},"agent_actions":{"view_html":"https://pith.science/pith/P67FHJ5DWMWTCIPKCDN7GHP7VM","download_json":"https://pith.science/pith/P67FHJ5DWMWTCIPKCDN7GHP7VM.json","view_paper":"https://pith.science/paper/P67FHJ5D","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2105.01679&json=true","fetch_graph":"https://pith.science/api/pith-number/P67FHJ5DWMWTCIPKCDN7GHP7VM/graph.json","fetch_events":"https://pith.science/api/pith-number/P67FHJ5DWMWTCIPKCDN7GHP7VM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/P67FHJ5DWMWTCIPKCDN7GHP7VM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/P67FHJ5DWMWTCIPKCDN7GHP7VM/action/storage_attestation","attest_author":"https://pith.science/pith/P67FHJ5DWMWTCIPKCDN7GHP7VM/action/author_attestation","sign_citation":"https://pith.science/pith/P67FHJ5DWMWTCIPKCDN7GHP7VM/action/citation_signature","submit_replication":"https://pith.science/pith/P67FHJ5DWMWTCIPKCDN7GHP7VM/action/replication_record"}},"created_at":"2026-07-05T05:26:01.467411+00:00","updated_at":"2026-07-05T05:26:01.467411+00:00"}