{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:NB4Z7V3UHUS4BKKCX6V4ZZ4GHD","short_pith_number":"pith:NB4Z7V3U","schema_version":"1.0","canonical_sha256":"68799fd7743d25c0a942bfabcce78638fe7fcca184ef2c7dc8a5d88faafcf0fc","source":{"kind":"arxiv","id":"1604.02191","version":2},"attestation_state":"computed","paper":{"title":"A new approach to the Higgs transverse-momentum resummation at NNLL+NNLO","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Emanuele Re, Paolo Torrielli, Pier Francesco Monni","submitted_at":"2016-04-07T22:54:25Z","abstract_excerpt":"We propose a new approach to the resummation of the transverse-momentum distribution of a high-mass colour-singlet system in hadronic collisions. The resummation is performed in momentum space and is free of kinematic singularities at small transverse momentum. We derive a formula accurate at the next-to-next-to-leading-logarithmic level, and present the first matched predictions to next-to-next-to-leading order for Higgs-boson production in gluon fusion at the LHC. This method can be adapted to all observables featuring kinematic cancellations in the infrared region."},"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":"1604.02191","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-04-07T22:54:25Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"6084945378acb37b2c1ff5ad3e1c7ffde650eb3d3aa142fa846410a2459c9e9c","abstract_canon_sha256":"dfc56d816e45f57cf32788f47b4b82e511c65fb26160d3cbc4e9e3add7c24526"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:12:03.962033Z","signature_b64":"wuhSYkJhphe23IYoeP60lF43sutaNAzp7GuWEfjQ76WMkx3tbTKxG2YhOQ9kanpaDae8WV5R9n3Aihga05MIDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"68799fd7743d25c0a942bfabcce78638fe7fcca184ef2c7dc8a5d88faafcf0fc","last_reissued_at":"2026-05-18T01:12:03.961706Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:12:03.961706Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A new approach to the Higgs transverse-momentum resummation at NNLL+NNLO","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Emanuele Re, Paolo Torrielli, Pier Francesco Monni","submitted_at":"2016-04-07T22:54:25Z","abstract_excerpt":"We propose a new approach to the resummation of the transverse-momentum distribution of a high-mass colour-singlet system in hadronic collisions. The resummation is performed in momentum space and is free of kinematic singularities at small transverse momentum. We derive a formula accurate at the next-to-next-to-leading-logarithmic level, and present the first matched predictions to next-to-next-to-leading order for Higgs-boson production in gluon fusion at the LHC. This method can be adapted to all observables featuring kinematic cancellations in the infrared region."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.02191","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":"1604.02191","created_at":"2026-05-18T01:12:03.961760+00:00"},{"alias_kind":"arxiv_version","alias_value":"1604.02191v2","created_at":"2026-05-18T01:12:03.961760+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.02191","created_at":"2026-05-18T01:12:03.961760+00:00"},{"alias_kind":"pith_short_12","alias_value":"NB4Z7V3UHUS4","created_at":"2026-05-18T12:30:32.724797+00:00"},{"alias_kind":"pith_short_16","alias_value":"NB4Z7V3UHUS4BKKC","created_at":"2026-05-18T12:30:32.724797+00:00"},{"alias_kind":"pith_short_8","alias_value":"NB4Z7V3U","created_at":"2026-05-18T12:30:32.724797+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"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":62,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NB4Z7V3UHUS4BKKCX6V4ZZ4GHD","json":"https://pith.science/pith/NB4Z7V3UHUS4BKKCX6V4ZZ4GHD.json","graph_json":"https://pith.science/api/pith-number/NB4Z7V3UHUS4BKKCX6V4ZZ4GHD/graph.json","events_json":"https://pith.science/api/pith-number/NB4Z7V3UHUS4BKKCX6V4ZZ4GHD/events.json","paper":"https://pith.science/paper/NB4Z7V3U"},"agent_actions":{"view_html":"https://pith.science/pith/NB4Z7V3UHUS4BKKCX6V4ZZ4GHD","download_json":"https://pith.science/pith/NB4Z7V3UHUS4BKKCX6V4ZZ4GHD.json","view_paper":"https://pith.science/paper/NB4Z7V3U","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1604.02191&json=true","fetch_graph":"https://pith.science/api/pith-number/NB4Z7V3UHUS4BKKCX6V4ZZ4GHD/graph.json","fetch_events":"https://pith.science/api/pith-number/NB4Z7V3UHUS4BKKCX6V4ZZ4GHD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NB4Z7V3UHUS4BKKCX6V4ZZ4GHD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NB4Z7V3UHUS4BKKCX6V4ZZ4GHD/action/storage_attestation","attest_author":"https://pith.science/pith/NB4Z7V3UHUS4BKKCX6V4ZZ4GHD/action/author_attestation","sign_citation":"https://pith.science/pith/NB4Z7V3UHUS4BKKCX6V4ZZ4GHD/action/citation_signature","submit_replication":"https://pith.science/pith/NB4Z7V3UHUS4BKKCX6V4ZZ4GHD/action/replication_record"}},"created_at":"2026-05-18T01:12:03.961760+00:00","updated_at":"2026-05-18T01:12:03.961760+00:00"}