{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:R4DEM52GZXMFYOGOFEW5QETKYZ","short_pith_number":"pith:R4DEM52G","schema_version":"1.0","canonical_sha256":"8f06467746cdd85c38ce292dd8126ac65c4bdefdf9de0850ae218c69d2f93a93","source":{"kind":"arxiv","id":"2111.05357","version":1},"attestation_state":"computed","paper":{"title":"QED Parton Distribution Functions in the MSHT20 Fit","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"A. D. Martin, L. A. Harland-Lang, R.S. Thorne, T. Cridge","submitted_at":"2021-11-09T19:02:32Z","abstract_excerpt":"We present the MSHT20qed set of parton distribution functions (PDFs). These are obtained from the MSHT20 global analysis via a refit including QED corrections to the DGLAP evolution at ${\\cal O}(\\alpha),{\\cal O}(\\alpha\\alpha_S)$ and ${\\cal O}(\\alpha^2)$, and containing the photon PDF of the proton. As in the previous MMHT15qed study we use an input distribution for the photon that is derived from the LUXqed formulation, and find good consistency for the photon PDF with that of MMHT15qed, as well as with other recent sets. We also present a set of QED corrected neutron PDFs and accompanying pho"},"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":"2111.05357","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2021-11-09T19:02:32Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"2fbaf4289e92d467cb22a998d2322f9c5aeb0f02de7a576f4e2bb6d004357cdf","abstract_canon_sha256":"f65c81687a7a2e9362d4e3ac531b0a044e5cf81f043d80bf76d1aec49e28a185"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:57:15.912174Z","signature_b64":"CWUieHxLFSndgAwMLUFwRnXtZOdQzgUHcYWFHLc6dTpkIYTC4CsL6pI0R2GR6kAPkScwQaOa30IdWGO+Fl2RDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8f06467746cdd85c38ce292dd8126ac65c4bdefdf9de0850ae218c69d2f93a93","last_reissued_at":"2026-07-05T03:57:15.911691Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:57:15.911691Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"QED Parton Distribution Functions in the MSHT20 Fit","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"A. D. Martin, L. A. Harland-Lang, R.S. Thorne, T. Cridge","submitted_at":"2021-11-09T19:02:32Z","abstract_excerpt":"We present the MSHT20qed set of parton distribution functions (PDFs). These are obtained from the MSHT20 global analysis via a refit including QED corrections to the DGLAP evolution at ${\\cal O}(\\alpha),{\\cal O}(\\alpha\\alpha_S)$ and ${\\cal O}(\\alpha^2)$, and containing the photon PDF of the proton. As in the previous MMHT15qed study we use an input distribution for the photon that is derived from the LUXqed formulation, and find good consistency for the photon PDF with that of MMHT15qed, as well as with other recent sets. We also present a set of QED corrected neutron PDFs and accompanying pho"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2111.05357","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/2111.05357/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":"2111.05357","created_at":"2026-07-05T03:57:15.911747+00:00"},{"alias_kind":"arxiv_version","alias_value":"2111.05357v1","created_at":"2026-07-05T03:57:15.911747+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2111.05357","created_at":"2026-07-05T03:57:15.911747+00:00"},{"alias_kind":"pith_short_12","alias_value":"R4DEM52GZXMF","created_at":"2026-07-05T03:57:15.911747+00:00"},{"alias_kind":"pith_short_16","alias_value":"R4DEM52GZXMFYOGO","created_at":"2026-07-05T03:57:15.911747+00:00"},{"alias_kind":"pith_short_8","alias_value":"R4DEM52G","created_at":"2026-07-05T03:57:15.911747+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.07664","citing_title":"Single inclusive hadron and jet production in lepton-hadron scattering","ref_index":29,"is_internal_anchor":true},{"citing_arxiv_id":"2504.06689","citing_title":"Les Houches 2023 -- Physics at TeV Colliders: Report on the Standard Model Precision Wishlist","ref_index":32,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/R4DEM52GZXMFYOGOFEW5QETKYZ","json":"https://pith.science/pith/R4DEM52GZXMFYOGOFEW5QETKYZ.json","graph_json":"https://pith.science/api/pith-number/R4DEM52GZXMFYOGOFEW5QETKYZ/graph.json","events_json":"https://pith.science/api/pith-number/R4DEM52GZXMFYOGOFEW5QETKYZ/events.json","paper":"https://pith.science/paper/R4DEM52G"},"agent_actions":{"view_html":"https://pith.science/pith/R4DEM52GZXMFYOGOFEW5QETKYZ","download_json":"https://pith.science/pith/R4DEM52GZXMFYOGOFEW5QETKYZ.json","view_paper":"https://pith.science/paper/R4DEM52G","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2111.05357&json=true","fetch_graph":"https://pith.science/api/pith-number/R4DEM52GZXMFYOGOFEW5QETKYZ/graph.json","fetch_events":"https://pith.science/api/pith-number/R4DEM52GZXMFYOGOFEW5QETKYZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/R4DEM52GZXMFYOGOFEW5QETKYZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/R4DEM52GZXMFYOGOFEW5QETKYZ/action/storage_attestation","attest_author":"https://pith.science/pith/R4DEM52GZXMFYOGOFEW5QETKYZ/action/author_attestation","sign_citation":"https://pith.science/pith/R4DEM52GZXMFYOGOFEW5QETKYZ/action/citation_signature","submit_replication":"https://pith.science/pith/R4DEM52GZXMFYOGOFEW5QETKYZ/action/replication_record"}},"created_at":"2026-07-05T03:57:15.911747+00:00","updated_at":"2026-07-05T03:57:15.911747+00:00"}