{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:7A7CPXZLOISJ3YVFPPP4V2LPWZ","short_pith_number":"pith:7A7CPXZL","schema_version":"1.0","canonical_sha256":"f83e27df2b72249de2a57bdfcae96fb67a3b9cfa7e9219c6a241876f4e7252c1","source":{"kind":"arxiv","id":"1801.06851","version":3},"attestation_state":"computed","paper":{"title":"Next-to-leading order QCD and electroweak corrections to Higgs-strahlung processes at the LHC","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ablikim Tursun, Nijat Yalkun, Pazilet Obul, Sayipjamal Dulat, Tie-Jiun Hou","submitted_at":"2018-01-21T16:59:22Z","abstract_excerpt":"In this paper we calculate the total and fiducial cross sections as well as differential distributions for the Higgs-strahlung or VH process $p p \\to VH \\to l\\nu_l/l^- l^+ + H$, (V = W or Z, l=e,$\\mu$) including QCD and electro-weak corrections up to next-to-leading order before and after reweighting photon PDFs of NNPDF2.3qed, NNPDF3.0qed, MRST2004qed, CT14QEDinc, and LUXqed at the LHC with 13 TeV and Higgs boson mass $\\ M_{H}=125$ GeV. The predictions from the various photon PDFs before and after reweighting against each other are in good agreement. The photon PDF uncertainties of the photon"},"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":"1801.06851","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"hep-ph","submitted_at":"2018-01-21T16:59:22Z","cross_cats_sorted":[],"title_canon_sha256":"cedea1f4c5f2df2371744079c8b2b62c4db512c1af2f218c912ac03eb7bd965d","abstract_canon_sha256":"2045fe8586cb872fba28f173e6d1b73d7516af70876de37fb35d5aab9c54283f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:01:09.900846Z","signature_b64":"M0p4d3Sh5O7KBASprk0CZH/LEsuXnwzj4dxAuoFv2BGtmRfrbiM/wcq/w6GrWCFh6SDxoPaRsVeLZ/cooOrxDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f83e27df2b72249de2a57bdfcae96fb67a3b9cfa7e9219c6a241876f4e7252c1","last_reissued_at":"2026-05-18T00:01:09.900194Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:01:09.900194Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Next-to-leading order QCD and electroweak corrections to Higgs-strahlung processes at the LHC","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ablikim Tursun, Nijat Yalkun, Pazilet Obul, Sayipjamal Dulat, Tie-Jiun Hou","submitted_at":"2018-01-21T16:59:22Z","abstract_excerpt":"In this paper we calculate the total and fiducial cross sections as well as differential distributions for the Higgs-strahlung or VH process $p p \\to VH \\to l\\nu_l/l^- l^+ + H$, (V = W or Z, l=e,$\\mu$) including QCD and electro-weak corrections up to next-to-leading order before and after reweighting photon PDFs of NNPDF2.3qed, NNPDF3.0qed, MRST2004qed, CT14QEDinc, and LUXqed at the LHC with 13 TeV and Higgs boson mass $\\ M_{H}=125$ GeV. The predictions from the various photon PDFs before and after reweighting against each other are in good agreement. The photon PDF uncertainties of the photon"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.06851","kind":"arxiv","version":3},"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":"1801.06851","created_at":"2026-05-18T00:01:09.900291+00:00"},{"alias_kind":"arxiv_version","alias_value":"1801.06851v3","created_at":"2026-05-18T00:01:09.900291+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.06851","created_at":"2026-05-18T00:01:09.900291+00:00"},{"alias_kind":"pith_short_12","alias_value":"7A7CPXZLOISJ","created_at":"2026-05-18T12:32:11.075285+00:00"},{"alias_kind":"pith_short_16","alias_value":"7A7CPXZLOISJ3YVF","created_at":"2026-05-18T12:32:11.075285+00:00"},{"alias_kind":"pith_short_8","alias_value":"7A7CPXZL","created_at":"2026-05-18T12:32:11.075285+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.27314","citing_title":"Planar master integrals for two-loop NLO electroweak light-fermion contributions to $g g \\rightarrow Z H$","ref_index":15,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7A7CPXZLOISJ3YVFPPP4V2LPWZ","json":"https://pith.science/pith/7A7CPXZLOISJ3YVFPPP4V2LPWZ.json","graph_json":"https://pith.science/api/pith-number/7A7CPXZLOISJ3YVFPPP4V2LPWZ/graph.json","events_json":"https://pith.science/api/pith-number/7A7CPXZLOISJ3YVFPPP4V2LPWZ/events.json","paper":"https://pith.science/paper/7A7CPXZL"},"agent_actions":{"view_html":"https://pith.science/pith/7A7CPXZLOISJ3YVFPPP4V2LPWZ","download_json":"https://pith.science/pith/7A7CPXZLOISJ3YVFPPP4V2LPWZ.json","view_paper":"https://pith.science/paper/7A7CPXZL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1801.06851&json=true","fetch_graph":"https://pith.science/api/pith-number/7A7CPXZLOISJ3YVFPPP4V2LPWZ/graph.json","fetch_events":"https://pith.science/api/pith-number/7A7CPXZLOISJ3YVFPPP4V2LPWZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7A7CPXZLOISJ3YVFPPP4V2LPWZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7A7CPXZLOISJ3YVFPPP4V2LPWZ/action/storage_attestation","attest_author":"https://pith.science/pith/7A7CPXZLOISJ3YVFPPP4V2LPWZ/action/author_attestation","sign_citation":"https://pith.science/pith/7A7CPXZLOISJ3YVFPPP4V2LPWZ/action/citation_signature","submit_replication":"https://pith.science/pith/7A7CPXZLOISJ3YVFPPP4V2LPWZ/action/replication_record"}},"created_at":"2026-05-18T00:01:09.900291+00:00","updated_at":"2026-05-18T00:01:09.900291+00:00"}