{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:O4HKOA4ELFASZNKID5YT7CKXMS","short_pith_number":"pith:O4HKOA4E","schema_version":"1.0","canonical_sha256":"770ea7038459412cb5481f713f895764a5597f77317fcbc774c49b13ca64de1c","source":{"kind":"arxiv","id":"2107.09717","version":1},"attestation_state":"computed","paper":{"title":"Next-to SV resummed Drell-Yan cross section beyond leading-logarithm","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"A. H. Ajjath, Aparna Sankar, Pooja Mukherjee, Surabhi Tiwari, V. Ravindran","submitted_at":"2021-07-20T18:36:38Z","abstract_excerpt":"We present the resummed predictions for inclusive cross section for Drell-Yan (DY) production up to next-to-next-to leading logarithmic ($\\rm \\overline{ NNLL}$) accuracy taking into account both soft virtual (SV) and next-to SV (NSV) threshold logarithms. We restrict ourselves to resummed contributions only from quark anti-quark ($q \\bar q$) initiated channels. The resummation is performed in Mellin-$N$ space. We derive the $N$-dependent coefficients and the $N$-independent constants to desired accuracy for our study. The resummed results are matched through the minimal prescription procedure "},"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":"2107.09717","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2021-07-20T18:36:38Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"133192d64768d3566061d8326927f7567411799589137d79c2c9e98c5bae8929","abstract_canon_sha256":"1d2be42402ca1b66f10f9283d52d56706c165575235fb2e51a61f890db8be6db"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:13:31.316253Z","signature_b64":"8iSJv/tzi3wK54JVozhMWjolVKHnfMKTXAzcbzg6PcSmmzVKpxkOC2KJkw/zfPKWjoWq44ngr+l2obTytGloCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"770ea7038459412cb5481f713f895764a5597f77317fcbc774c49b13ca64de1c","last_reissued_at":"2026-07-05T04:13:31.315790Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:13:31.315790Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Next-to SV resummed Drell-Yan cross section beyond leading-logarithm","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"A. H. Ajjath, Aparna Sankar, Pooja Mukherjee, Surabhi Tiwari, V. Ravindran","submitted_at":"2021-07-20T18:36:38Z","abstract_excerpt":"We present the resummed predictions for inclusive cross section for Drell-Yan (DY) production up to next-to-next-to leading logarithmic ($\\rm \\overline{ NNLL}$) accuracy taking into account both soft virtual (SV) and next-to SV (NSV) threshold logarithms. We restrict ourselves to resummed contributions only from quark anti-quark ($q \\bar q$) initiated channels. The resummation is performed in Mellin-$N$ space. We derive the $N$-dependent coefficients and the $N$-independent constants to desired accuracy for our study. The resummed results are matched through the minimal prescription procedure "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2107.09717","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2107.09717/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":"2107.09717","created_at":"2026-07-05T04:13:31.315848+00:00"},{"alias_kind":"arxiv_version","alias_value":"2107.09717v1","created_at":"2026-07-05T04:13:31.315848+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2107.09717","created_at":"2026-07-05T04:13:31.315848+00:00"},{"alias_kind":"pith_short_12","alias_value":"O4HKOA4ELFAS","created_at":"2026-07-05T04:13:31.315848+00:00"},{"alias_kind":"pith_short_16","alias_value":"O4HKOA4ELFASZNKI","created_at":"2026-07-05T04:13:31.315848+00:00"},{"alias_kind":"pith_short_8","alias_value":"O4HKOA4E","created_at":"2026-07-05T04:13:31.315848+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2607.01413","citing_title":"One-loop matching of QCD currents to power-suppressed two-jet operators","ref_index":6,"is_internal_anchor":false},{"citing_arxiv_id":"2510.05584","citing_title":"NLP threshold corrections to W+jet production","ref_index":25,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/O4HKOA4ELFASZNKID5YT7CKXMS","json":"https://pith.science/pith/O4HKOA4ELFASZNKID5YT7CKXMS.json","graph_json":"https://pith.science/api/pith-number/O4HKOA4ELFASZNKID5YT7CKXMS/graph.json","events_json":"https://pith.science/api/pith-number/O4HKOA4ELFASZNKID5YT7CKXMS/events.json","paper":"https://pith.science/paper/O4HKOA4E"},"agent_actions":{"view_html":"https://pith.science/pith/O4HKOA4ELFASZNKID5YT7CKXMS","download_json":"https://pith.science/pith/O4HKOA4ELFASZNKID5YT7CKXMS.json","view_paper":"https://pith.science/paper/O4HKOA4E","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2107.09717&json=true","fetch_graph":"https://pith.science/api/pith-number/O4HKOA4ELFASZNKID5YT7CKXMS/graph.json","fetch_events":"https://pith.science/api/pith-number/O4HKOA4ELFASZNKID5YT7CKXMS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/O4HKOA4ELFASZNKID5YT7CKXMS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/O4HKOA4ELFASZNKID5YT7CKXMS/action/storage_attestation","attest_author":"https://pith.science/pith/O4HKOA4ELFASZNKID5YT7CKXMS/action/author_attestation","sign_citation":"https://pith.science/pith/O4HKOA4ELFASZNKID5YT7CKXMS/action/citation_signature","submit_replication":"https://pith.science/pith/O4HKOA4ELFASZNKID5YT7CKXMS/action/replication_record"}},"created_at":"2026-07-05T04:13:31.315848+00:00","updated_at":"2026-07-05T04:13:31.315848+00:00"}