{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:FOZHIIQHJP7ZEGWFL3FXKJSTVG","short_pith_number":"pith:FOZHIIQH","schema_version":"1.0","canonical_sha256":"2bb27422074bff921ac55ecb752653a99dcc2d4f339cf5c104eca980e802596e","source":{"kind":"arxiv","id":"1402.5032","version":2},"attestation_state":"computed","paper":{"title":"Two-loop fermion self-energy and propagator in reduced QED$_{3,2}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","hep-th"],"primary_cat":"hep-ph","authors_text":"S. Teber","submitted_at":"2014-02-20T15:25:29Z","abstract_excerpt":"We compute the two-loop fermion self-energy in massless reduced quantum electrodynamics (RQED) for an arbitrary gauge in the case where the photon field is three-dimensional and the fermion field two-dimensional: super-renormalizable RQED$_{3,2}$ with $N_F$ fermions. We find that the theory is infrared finite at two-loop and that finite corrections to the fermion propagator have a remarkably simple form."},"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":"1402.5032","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-02-20T15:25:29Z","cross_cats_sorted":["cond-mat.mes-hall","hep-th"],"title_canon_sha256":"6ef18df26989bf5be6a9c77ff64ede4775ee8b96c026b113c0442e68e7855882","abstract_canon_sha256":"48094946ad22da4d138933d73a768d1972d2ee036d84c1dc9ef01c58870b3939"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:55:12.962893Z","signature_b64":"fn3t2Wbbmp6F2y5NevWio3tsS8vAvScfsskcOWmWqTG9TY9jieHGTLDWVQ99uT9acycXyIihmtmd5FVCcO5FBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2bb27422074bff921ac55ecb752653a99dcc2d4f339cf5c104eca980e802596e","last_reissued_at":"2026-05-18T02:55:12.962495Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:55:12.962495Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Two-loop fermion self-energy and propagator in reduced QED$_{3,2}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","hep-th"],"primary_cat":"hep-ph","authors_text":"S. Teber","submitted_at":"2014-02-20T15:25:29Z","abstract_excerpt":"We compute the two-loop fermion self-energy in massless reduced quantum electrodynamics (RQED) for an arbitrary gauge in the case where the photon field is three-dimensional and the fermion field two-dimensional: super-renormalizable RQED$_{3,2}$ with $N_F$ fermions. We find that the theory is infrared finite at two-loop and that finite corrections to the fermion propagator have a remarkably simple form."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.5032","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":""},"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":"1402.5032","created_at":"2026-05-18T02:55:12.962557+00:00"},{"alias_kind":"arxiv_version","alias_value":"1402.5032v2","created_at":"2026-05-18T02:55:12.962557+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.5032","created_at":"2026-05-18T02:55:12.962557+00:00"},{"alias_kind":"pith_short_12","alias_value":"FOZHIIQHJP7Z","created_at":"2026-05-18T12:28:28.263976+00:00"},{"alias_kind":"pith_short_16","alias_value":"FOZHIIQHJP7ZEGWF","created_at":"2026-05-18T12:28:28.263976+00:00"},{"alias_kind":"pith_short_8","alias_value":"FOZHIIQH","created_at":"2026-05-18T12:28:28.263976+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.14122","citing_title":"Landau-Khalatnikov-Fradkin Transformations in Reduced Quantum Electrodynamics: Perturbative and Nonperturbative Dynamics of the Fermion Propagator","ref_index":15,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FOZHIIQHJP7ZEGWFL3FXKJSTVG","json":"https://pith.science/pith/FOZHIIQHJP7ZEGWFL3FXKJSTVG.json","graph_json":"https://pith.science/api/pith-number/FOZHIIQHJP7ZEGWFL3FXKJSTVG/graph.json","events_json":"https://pith.science/api/pith-number/FOZHIIQHJP7ZEGWFL3FXKJSTVG/events.json","paper":"https://pith.science/paper/FOZHIIQH"},"agent_actions":{"view_html":"https://pith.science/pith/FOZHIIQHJP7ZEGWFL3FXKJSTVG","download_json":"https://pith.science/pith/FOZHIIQHJP7ZEGWFL3FXKJSTVG.json","view_paper":"https://pith.science/paper/FOZHIIQH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1402.5032&json=true","fetch_graph":"https://pith.science/api/pith-number/FOZHIIQHJP7ZEGWFL3FXKJSTVG/graph.json","fetch_events":"https://pith.science/api/pith-number/FOZHIIQHJP7ZEGWFL3FXKJSTVG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FOZHIIQHJP7ZEGWFL3FXKJSTVG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FOZHIIQHJP7ZEGWFL3FXKJSTVG/action/storage_attestation","attest_author":"https://pith.science/pith/FOZHIIQHJP7ZEGWFL3FXKJSTVG/action/author_attestation","sign_citation":"https://pith.science/pith/FOZHIIQHJP7ZEGWFL3FXKJSTVG/action/citation_signature","submit_replication":"https://pith.science/pith/FOZHIIQHJP7ZEGWFL3FXKJSTVG/action/replication_record"}},"created_at":"2026-05-18T02:55:12.962557+00:00","updated_at":"2026-05-18T02:55:12.962557+00:00"}