{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:6AJRAHJ2HGENZSN4OXIJGL3SLY","short_pith_number":"pith:6AJRAHJ2","schema_version":"1.0","canonical_sha256":"f013101d3a3988dcc9bc75d0932f725e1c7d0ab132f8933c7afd21499c44023a","source":{"kind":"arxiv","id":"1612.00283","version":1},"attestation_state":"computed","paper":{"title":"Modeling BSM effects on the Higgs transverse-momentum spectrum in an EFT approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Agnieszka Ilnicka, Marius Wiesemann, Massimiliano Grazzini, Michael Spira","submitted_at":"2016-12-01T14:55:46Z","abstract_excerpt":"We consider the transverse-momentum distribution of a Higgs boson produced through gluon fusion in hadron collisions. At small transverse momenta, the large logarithmic terms are resummed up to next-to-leading-logarithmic (NLL) accuracy. The resummed computation is consistently matched to the next-to-leading-order (NLO) result valid at large transverse momenta. The ensuing Standard Model prediction is supplemented by possible new-physics effects parametrised through three dimension-six operators related to the modification of the top and bottom Yukawa couplings, and to the inclusion of a point"},"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":"1612.00283","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-12-01T14:55:46Z","cross_cats_sorted":[],"title_canon_sha256":"a9a7f279753c7714a7769278111037f8d29a84e9c39fcad97560a1127df42daa","abstract_canon_sha256":"f0eb0b19e5f5388d702741dc361a0e0bfedd5513322bfc0e76b719f9464e5bf0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:45:44.631051Z","signature_b64":"toPI1XxIvI6UlKvLTV7ida+cuO3INR5yfIcOGbtYwZ7qY3PnsJOAyrtnM6QSALUcN9/jJEm2Z54sCMEJ+ShIAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f013101d3a3988dcc9bc75d0932f725e1c7d0ab132f8933c7afd21499c44023a","last_reissued_at":"2026-05-18T00:45:44.630489Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:45:44.630489Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Modeling BSM effects on the Higgs transverse-momentum spectrum in an EFT approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Agnieszka Ilnicka, Marius Wiesemann, Massimiliano Grazzini, Michael Spira","submitted_at":"2016-12-01T14:55:46Z","abstract_excerpt":"We consider the transverse-momentum distribution of a Higgs boson produced through gluon fusion in hadron collisions. At small transverse momenta, the large logarithmic terms are resummed up to next-to-leading-logarithmic (NLL) accuracy. The resummed computation is consistently matched to the next-to-leading-order (NLO) result valid at large transverse momenta. The ensuing Standard Model prediction is supplemented by possible new-physics effects parametrised through three dimension-six operators related to the modification of the top and bottom Yukawa couplings, and to the inclusion of a point"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1612.00283","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":"1612.00283","created_at":"2026-05-18T00:45:44.630576+00:00"},{"alias_kind":"arxiv_version","alias_value":"1612.00283v1","created_at":"2026-05-18T00:45:44.630576+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1612.00283","created_at":"2026-05-18T00:45:44.630576+00:00"},{"alias_kind":"pith_short_12","alias_value":"6AJRAHJ2HGEN","created_at":"2026-05-18T12:30:01.593930+00:00"},{"alias_kind":"pith_short_16","alias_value":"6AJRAHJ2HGENZSN4","created_at":"2026-05-18T12:30:01.593930+00:00"},{"alias_kind":"pith_short_8","alias_value":"6AJRAHJ2","created_at":"2026-05-18T12:30:01.593930+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2504.13081","citing_title":"Combination and interpretation of differential Higgs boson production cross sections in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","ref_index":28,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6AJRAHJ2HGENZSN4OXIJGL3SLY","json":"https://pith.science/pith/6AJRAHJ2HGENZSN4OXIJGL3SLY.json","graph_json":"https://pith.science/api/pith-number/6AJRAHJ2HGENZSN4OXIJGL3SLY/graph.json","events_json":"https://pith.science/api/pith-number/6AJRAHJ2HGENZSN4OXIJGL3SLY/events.json","paper":"https://pith.science/paper/6AJRAHJ2"},"agent_actions":{"view_html":"https://pith.science/pith/6AJRAHJ2HGENZSN4OXIJGL3SLY","download_json":"https://pith.science/pith/6AJRAHJ2HGENZSN4OXIJGL3SLY.json","view_paper":"https://pith.science/paper/6AJRAHJ2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1612.00283&json=true","fetch_graph":"https://pith.science/api/pith-number/6AJRAHJ2HGENZSN4OXIJGL3SLY/graph.json","fetch_events":"https://pith.science/api/pith-number/6AJRAHJ2HGENZSN4OXIJGL3SLY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6AJRAHJ2HGENZSN4OXIJGL3SLY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6AJRAHJ2HGENZSN4OXIJGL3SLY/action/storage_attestation","attest_author":"https://pith.science/pith/6AJRAHJ2HGENZSN4OXIJGL3SLY/action/author_attestation","sign_citation":"https://pith.science/pith/6AJRAHJ2HGENZSN4OXIJGL3SLY/action/citation_signature","submit_replication":"https://pith.science/pith/6AJRAHJ2HGENZSN4OXIJGL3SLY/action/replication_record"}},"created_at":"2026-05-18T00:45:44.630576+00:00","updated_at":"2026-05-18T00:45:44.630576+00:00"}