{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:VXYQT7PHLB7TE2UUHBUTC7AWH2","short_pith_number":"pith:VXYQT7PH","schema_version":"1.0","canonical_sha256":"adf109fde7587f326a943869317c163ebb72ec58326ba2b6120f52695fed37be","source":{"kind":"arxiv","id":"2010.00079","version":2},"attestation_state":"computed","paper":{"title":"Next-to-soft corrections for Drell-Yan and Higgs boson rapidity distributions beyond N$^3$LO","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.H. Ajjath, Aparna Sankar, Pooja Mukherjee, Surabhi Tiwari, V. Ravindran","submitted_at":"2020-09-30T19:48:50Z","abstract_excerpt":"We present a formalism that sums up both soft-virtual (SV) and next to SV (NSV) contributions to all orders in perturbative QCD for the rapidity distribution of any colorless particle produced in hadron colliders. We have exploited the factorization properties and the renormalisation group (RG) invariance of the differential cross-section to achieve this. Using the state-of-the-art multiloop and multileg results, we determine the complete NSV contributions to third order in strong coupling constant for the rapidity distributions for a pair of leptons in Drell-Yan and also for Higgs boson in gl"},"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":"2010.00079","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2020-09-30T19:48:50Z","cross_cats_sorted":[],"title_canon_sha256":"02381e6c46d8b33b7c2941a2abd24fa587855198ab33bc4ac7d655cb6baa675e","abstract_canon_sha256":"f28e1ae822caf1152464f7416a32c9130e5935ca257f95e31344c97686950020"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:01:33.809896Z","signature_b64":"FwHN80jxgvsOeHp38wM8RjDEde2yYUIvyzy78MlFqDCJ3EmH7GkNbHAxGELV1yWbu3oTaDo7wfLiE+I3WeptBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"adf109fde7587f326a943869317c163ebb72ec58326ba2b6120f52695fed37be","last_reissued_at":"2026-07-05T03:01:33.809328Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:01:33.809328Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Next-to-soft corrections for Drell-Yan and Higgs boson rapidity distributions beyond N$^3$LO","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.H. Ajjath, Aparna Sankar, Pooja Mukherjee, Surabhi Tiwari, V. Ravindran","submitted_at":"2020-09-30T19:48:50Z","abstract_excerpt":"We present a formalism that sums up both soft-virtual (SV) and next to SV (NSV) contributions to all orders in perturbative QCD for the rapidity distribution of any colorless particle produced in hadron colliders. We have exploited the factorization properties and the renormalisation group (RG) invariance of the differential cross-section to achieve this. Using the state-of-the-art multiloop and multileg results, we determine the complete NSV contributions to third order in strong coupling constant for the rapidity distributions for a pair of leptons in Drell-Yan and also for Higgs boson in gl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2010.00079","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/2010.00079/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":"2010.00079","created_at":"2026-07-05T03:01:33.809408+00:00"},{"alias_kind":"arxiv_version","alias_value":"2010.00079v2","created_at":"2026-07-05T03:01:33.809408+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2010.00079","created_at":"2026-07-05T03:01:33.809408+00:00"},{"alias_kind":"pith_short_12","alias_value":"VXYQT7PHLB7T","created_at":"2026-07-05T03:01:33.809408+00:00"},{"alias_kind":"pith_short_16","alias_value":"VXYQT7PHLB7TE2UU","created_at":"2026-07-05T03:01:33.809408+00:00"},{"alias_kind":"pith_short_8","alias_value":"VXYQT7PH","created_at":"2026-07-05T03:01:33.809408+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2510.05584","citing_title":"NLP threshold corrections to W+jet production","ref_index":51,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VXYQT7PHLB7TE2UUHBUTC7AWH2","json":"https://pith.science/pith/VXYQT7PHLB7TE2UUHBUTC7AWH2.json","graph_json":"https://pith.science/api/pith-number/VXYQT7PHLB7TE2UUHBUTC7AWH2/graph.json","events_json":"https://pith.science/api/pith-number/VXYQT7PHLB7TE2UUHBUTC7AWH2/events.json","paper":"https://pith.science/paper/VXYQT7PH"},"agent_actions":{"view_html":"https://pith.science/pith/VXYQT7PHLB7TE2UUHBUTC7AWH2","download_json":"https://pith.science/pith/VXYQT7PHLB7TE2UUHBUTC7AWH2.json","view_paper":"https://pith.science/paper/VXYQT7PH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2010.00079&json=true","fetch_graph":"https://pith.science/api/pith-number/VXYQT7PHLB7TE2UUHBUTC7AWH2/graph.json","fetch_events":"https://pith.science/api/pith-number/VXYQT7PHLB7TE2UUHBUTC7AWH2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VXYQT7PHLB7TE2UUHBUTC7AWH2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VXYQT7PHLB7TE2UUHBUTC7AWH2/action/storage_attestation","attest_author":"https://pith.science/pith/VXYQT7PHLB7TE2UUHBUTC7AWH2/action/author_attestation","sign_citation":"https://pith.science/pith/VXYQT7PHLB7TE2UUHBUTC7AWH2/action/citation_signature","submit_replication":"https://pith.science/pith/VXYQT7PHLB7TE2UUHBUTC7AWH2/action/replication_record"}},"created_at":"2026-07-05T03:01:33.809408+00:00","updated_at":"2026-07-05T03:01:33.809408+00:00"}