{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:MAQFNYZVOR4T2ZYWND63PTDNJD","short_pith_number":"pith:MAQFNYZV","schema_version":"1.0","canonical_sha256":"602056e33574793d671668fdb7cc6d48e4a6b95e8fe39208ecac86530a031223","source":{"kind":"arxiv","id":"2102.07607","version":2},"attestation_state":"computed","paper":{"title":"Fully Differential Higgs Boson Production to Third Order in QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Huss, A. Pelloni, B. Mistlberger, E. W. N. Glover, T. Gehrmann, X. Chen","submitted_at":"2021-02-15T15:51:42Z","abstract_excerpt":"We present fully differential predictions for the production cross section of a Higgs boson via the gluon fusion mechanism at next-to-next-to-next-to leading order (N$^3$LO) in QCD perturbation theory. To perform our calculation we apply the Projection-to-Born method for the first time to the calculation of the non-factorising production of a colorless final state at the LHC at N$^3$LO. We predict differential distributions for the two photon final state produced by the decay of the Higgs boson and apply fiducial cuts on the photon rapidities and momenta. The N$^3$LO corrections to these diffe"},"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":"2102.07607","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2021-02-15T15:51:42Z","cross_cats_sorted":[],"title_canon_sha256":"f468a18b7a5e984a9e966c05786ea7b03373ee3bf87724793d629454d59523c5","abstract_canon_sha256":"830244d8fda4b76757e6c3417d8d547a9cdc5cbfdca5c57904d21cf9740b144f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:06:19.561929Z","signature_b64":"k+4KqxdbypPiW19Y+2ac/53U2XQ+Y9nm3w5+0GPFXISo8JeGSMw41B751Qs0Ol/18FkrIUxFwYTUG2xJGeLgAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"602056e33574793d671668fdb7cc6d48e4a6b95e8fe39208ecac86530a031223","last_reissued_at":"2026-07-05T03:06:19.561396Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:06:19.561396Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Fully Differential Higgs Boson Production to Third Order in QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Huss, A. Pelloni, B. Mistlberger, E. W. N. Glover, T. Gehrmann, X. Chen","submitted_at":"2021-02-15T15:51:42Z","abstract_excerpt":"We present fully differential predictions for the production cross section of a Higgs boson via the gluon fusion mechanism at next-to-next-to-next-to leading order (N$^3$LO) in QCD perturbation theory. To perform our calculation we apply the Projection-to-Born method for the first time to the calculation of the non-factorising production of a colorless final state at the LHC at N$^3$LO. We predict differential distributions for the two photon final state produced by the decay of the Higgs boson and apply fiducial cuts on the photon rapidities and momenta. The N$^3$LO corrections to these diffe"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2102.07607","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2102.07607/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":"2102.07607","created_at":"2026-07-05T03:06:19.561458+00:00"},{"alias_kind":"arxiv_version","alias_value":"2102.07607v2","created_at":"2026-07-05T03:06:19.561458+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2102.07607","created_at":"2026-07-05T03:06:19.561458+00:00"},{"alias_kind":"pith_short_12","alias_value":"MAQFNYZVOR4T","created_at":"2026-07-05T03:06:19.561458+00:00"},{"alias_kind":"pith_short_16","alias_value":"MAQFNYZVOR4T2ZYW","created_at":"2026-07-05T03:06:19.561458+00:00"},{"alias_kind":"pith_short_8","alias_value":"MAQFNYZV","created_at":"2026-07-05T03:06:19.561458+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.31286","citing_title":"Boosted Higgs-strahlung off a $W$ boson at next-to-next-to-next-to-leading order in QCD","ref_index":41,"is_internal_anchor":false},{"citing_arxiv_id":"2411.11846","citing_title":"Emergence of Calabi-Yau manifolds in high-precision black hole scattering","ref_index":46,"is_internal_anchor":false},{"citing_arxiv_id":"2604.12613","citing_title":"Next-to-next-to-next-to-leading order QCD corrections to photon-pair production","ref_index":39,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MAQFNYZVOR4T2ZYWND63PTDNJD","json":"https://pith.science/pith/MAQFNYZVOR4T2ZYWND63PTDNJD.json","graph_json":"https://pith.science/api/pith-number/MAQFNYZVOR4T2ZYWND63PTDNJD/graph.json","events_json":"https://pith.science/api/pith-number/MAQFNYZVOR4T2ZYWND63PTDNJD/events.json","paper":"https://pith.science/paper/MAQFNYZV"},"agent_actions":{"view_html":"https://pith.science/pith/MAQFNYZVOR4T2ZYWND63PTDNJD","download_json":"https://pith.science/pith/MAQFNYZVOR4T2ZYWND63PTDNJD.json","view_paper":"https://pith.science/paper/MAQFNYZV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2102.07607&json=true","fetch_graph":"https://pith.science/api/pith-number/MAQFNYZVOR4T2ZYWND63PTDNJD/graph.json","fetch_events":"https://pith.science/api/pith-number/MAQFNYZVOR4T2ZYWND63PTDNJD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MAQFNYZVOR4T2ZYWND63PTDNJD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MAQFNYZVOR4T2ZYWND63PTDNJD/action/storage_attestation","attest_author":"https://pith.science/pith/MAQFNYZVOR4T2ZYWND63PTDNJD/action/author_attestation","sign_citation":"https://pith.science/pith/MAQFNYZVOR4T2ZYWND63PTDNJD/action/citation_signature","submit_replication":"https://pith.science/pith/MAQFNYZVOR4T2ZYWND63PTDNJD/action/replication_record"}},"created_at":"2026-07-05T03:06:19.561458+00:00","updated_at":"2026-07-05T03:06:19.561458+00:00"}