{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:T2NLQT2BRLKMWN5OGO73MLBIQW","short_pith_number":"pith:T2NLQT2B","schema_version":"1.0","canonical_sha256":"9e9ab84f418ad4cb37ae33bfb62c288584fc3bfdd086e860f2cc3c1cae4ee53d","source":{"kind":"arxiv","id":"1105.4359","version":1},"attestation_state":"computed","paper":{"title":"Generalization of radiative jet energy loss to non-zero magnetic mass","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Magdalena Djordjevic, Marko Djordjevic","submitted_at":"2011-05-22T18:39:43Z","abstract_excerpt":"Reliable predictions for jet quenching in ultra-relativistic heavy ion collisions require accurate computation of radiative energy loss. With this goal, an energy loss formalism in a realistic finite size dynamical QCD medium was recently developed. While this formalism assumes zero magnetic mass - in accordance with the one-loop perturbative calculations - different non-perturbative approaches report a non-zero magnetic mass at RHIC and LHC. We here generalize the energy loss to consistently include a possibility for existence of non-zero magnetic screening. We also present how the inclusion "},"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":"1105.4359","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2011-05-22T18:39:43Z","cross_cats_sorted":[],"title_canon_sha256":"fc697e3d1c2cb032515a5915961147543b224bfebea41ea67d625df04304a7a0","abstract_canon_sha256":"5390c790103e3e01a25c466a2ec0d25fbcf9fdbee36ba8074e08fcae3dd356d1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:01:52.943793Z","signature_b64":"IsMjAEMhcms+QvuZZg3O1koRyNTBOzH5QhNqEmw9Tje97yX1XG2pZ3w+8h5X7FZrFVtKJ/TUE4+h4PZF4uR9Dw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9e9ab84f418ad4cb37ae33bfb62c288584fc3bfdd086e860f2cc3c1cae4ee53d","last_reissued_at":"2026-05-18T02:01:52.943099Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:01:52.943099Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Generalization of radiative jet energy loss to non-zero magnetic mass","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Magdalena Djordjevic, Marko Djordjevic","submitted_at":"2011-05-22T18:39:43Z","abstract_excerpt":"Reliable predictions for jet quenching in ultra-relativistic heavy ion collisions require accurate computation of radiative energy loss. With this goal, an energy loss formalism in a realistic finite size dynamical QCD medium was recently developed. While this formalism assumes zero magnetic mass - in accordance with the one-loop perturbative calculations - different non-perturbative approaches report a non-zero magnetic mass at RHIC and LHC. We here generalize the energy loss to consistently include a possibility for existence of non-zero magnetic screening. We also present how the inclusion "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.4359","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":""},"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":"1105.4359","created_at":"2026-05-18T02:01:52.943199+00:00"},{"alias_kind":"arxiv_version","alias_value":"1105.4359v1","created_at":"2026-05-18T02:01:52.943199+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.4359","created_at":"2026-05-18T02:01:52.943199+00:00"},{"alias_kind":"pith_short_12","alias_value":"T2NLQT2BRLKM","created_at":"2026-05-18T12:26:41.206345+00:00"},{"alias_kind":"pith_short_16","alias_value":"T2NLQT2BRLKMWN5O","created_at":"2026-05-18T12:26:41.206345+00:00"},{"alias_kind":"pith_short_8","alias_value":"T2NLQT2B","created_at":"2026-05-18T12:26:41.206345+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/T2NLQT2BRLKMWN5OGO73MLBIQW","json":"https://pith.science/pith/T2NLQT2BRLKMWN5OGO73MLBIQW.json","graph_json":"https://pith.science/api/pith-number/T2NLQT2BRLKMWN5OGO73MLBIQW/graph.json","events_json":"https://pith.science/api/pith-number/T2NLQT2BRLKMWN5OGO73MLBIQW/events.json","paper":"https://pith.science/paper/T2NLQT2B"},"agent_actions":{"view_html":"https://pith.science/pith/T2NLQT2BRLKMWN5OGO73MLBIQW","download_json":"https://pith.science/pith/T2NLQT2BRLKMWN5OGO73MLBIQW.json","view_paper":"https://pith.science/paper/T2NLQT2B","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1105.4359&json=true","fetch_graph":"https://pith.science/api/pith-number/T2NLQT2BRLKMWN5OGO73MLBIQW/graph.json","fetch_events":"https://pith.science/api/pith-number/T2NLQT2BRLKMWN5OGO73MLBIQW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/T2NLQT2BRLKMWN5OGO73MLBIQW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/T2NLQT2BRLKMWN5OGO73MLBIQW/action/storage_attestation","attest_author":"https://pith.science/pith/T2NLQT2BRLKMWN5OGO73MLBIQW/action/author_attestation","sign_citation":"https://pith.science/pith/T2NLQT2BRLKMWN5OGO73MLBIQW/action/citation_signature","submit_replication":"https://pith.science/pith/T2NLQT2BRLKMWN5OGO73MLBIQW/action/replication_record"}},"created_at":"2026-05-18T02:01:52.943199+00:00","updated_at":"2026-05-18T02:01:52.943199+00:00"}