{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:V6FYVF7HIOLEK4O43VQFCX3MFB","short_pith_number":"pith:V6FYVF7H","schema_version":"1.0","canonical_sha256":"af8b8a97e743964571dcdd60515f6c2852849d9dc1cf117ff936c33b9c7217cf","source":{"kind":"arxiv","id":"1411.5301","version":1},"attestation_state":"computed","paper":{"title":"Higgs Rapidity Distribution in $b {\\bar b}$ Annihilation at Threshold in N$^{3}$LO QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"M. K. Mandal, Narayan Rana, Taushif Ahmed, V. Ravindran","submitted_at":"2014-11-19T18:21:10Z","abstract_excerpt":"We present the rapidity distribution of the Higgs boson produced through bottom quark annihilation at third order in QCD using the threshold approximation. We provide a framework, based on the factorization properties of the QCD amplitudes along with Sudakov resummation and the renormalization group invariance, that allows one to perform the computation of the threshold corrections in a consistent, systematic and accurate way. The recent results on threshold N$^3$LO correction in QCD for the Drell-Yan production and on three loop QCD correction to Higgs form factor with bottom anti-bottom quar"},"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":"1411.5301","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-11-19T18:21:10Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"8e96732fe1845c94beaee142ca64f4dd0d493c13489ced6531800e83ad91a38e","abstract_canon_sha256":"f9bfc1ddac35c0ce97a144b22fbf636e66d8c315d3dd517a70d844b15e960e46"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:29.065136Z","signature_b64":"z8N8CI+mUltwB6WTNAOO+/qIcsGboG2F2PwkKG4AABe0ma/9qVOHIetxods1eZrZi+FCw7e8YMzbM+YC+6xQCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"af8b8a97e743964571dcdd60515f6c2852849d9dc1cf117ff936c33b9c7217cf","last_reissued_at":"2026-05-18T01:41:29.064669Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:29.064669Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higgs Rapidity Distribution in $b {\\bar b}$ Annihilation at Threshold in N$^{3}$LO QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"M. K. Mandal, Narayan Rana, Taushif Ahmed, V. Ravindran","submitted_at":"2014-11-19T18:21:10Z","abstract_excerpt":"We present the rapidity distribution of the Higgs boson produced through bottom quark annihilation at third order in QCD using the threshold approximation. We provide a framework, based on the factorization properties of the QCD amplitudes along with Sudakov resummation and the renormalization group invariance, that allows one to perform the computation of the threshold corrections in a consistent, systematic and accurate way. The recent results on threshold N$^3$LO correction in QCD for the Drell-Yan production and on three loop QCD correction to Higgs form factor with bottom anti-bottom quar"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.5301","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":"1411.5301","created_at":"2026-05-18T01:41:29.064737+00:00"},{"alias_kind":"arxiv_version","alias_value":"1411.5301v1","created_at":"2026-05-18T01:41:29.064737+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.5301","created_at":"2026-05-18T01:41:29.064737+00:00"},{"alias_kind":"pith_short_12","alias_value":"V6FYVF7HIOLE","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_16","alias_value":"V6FYVF7HIOLEK4O4","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_8","alias_value":"V6FYVF7H","created_at":"2026-05-18T12:28:52.271510+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/V6FYVF7HIOLEK4O43VQFCX3MFB","json":"https://pith.science/pith/V6FYVF7HIOLEK4O43VQFCX3MFB.json","graph_json":"https://pith.science/api/pith-number/V6FYVF7HIOLEK4O43VQFCX3MFB/graph.json","events_json":"https://pith.science/api/pith-number/V6FYVF7HIOLEK4O43VQFCX3MFB/events.json","paper":"https://pith.science/paper/V6FYVF7H"},"agent_actions":{"view_html":"https://pith.science/pith/V6FYVF7HIOLEK4O43VQFCX3MFB","download_json":"https://pith.science/pith/V6FYVF7HIOLEK4O43VQFCX3MFB.json","view_paper":"https://pith.science/paper/V6FYVF7H","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1411.5301&json=true","fetch_graph":"https://pith.science/api/pith-number/V6FYVF7HIOLEK4O43VQFCX3MFB/graph.json","fetch_events":"https://pith.science/api/pith-number/V6FYVF7HIOLEK4O43VQFCX3MFB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/V6FYVF7HIOLEK4O43VQFCX3MFB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/V6FYVF7HIOLEK4O43VQFCX3MFB/action/storage_attestation","attest_author":"https://pith.science/pith/V6FYVF7HIOLEK4O43VQFCX3MFB/action/author_attestation","sign_citation":"https://pith.science/pith/V6FYVF7HIOLEK4O43VQFCX3MFB/action/citation_signature","submit_replication":"https://pith.science/pith/V6FYVF7HIOLEK4O43VQFCX3MFB/action/replication_record"}},"created_at":"2026-05-18T01:41:29.064737+00:00","updated_at":"2026-05-18T01:41:29.064737+00:00"}