{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:NSMWOKKCFAJTIDUG73EMVK5MR5","short_pith_number":"pith:NSMWOKKC","schema_version":"1.0","canonical_sha256":"6c996729422813340e86fec8caabac8f778fd4fd66e59797e82eaef8201de60b","source":{"kind":"arxiv","id":"1805.11322","version":2},"attestation_state":"computed","paper":{"title":"Neutralino/chargino pair production at NLO+NLL with resummation-improved PDFs for LHC Run II","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"J. Fiaschi, M. Klasen","submitted_at":"2018-05-29T09:26:46Z","abstract_excerpt":"We make use of recently released parton density functions (PDFs) with threshold-resummation improvement to consistently calculate theoretical predictions for neutralino and chargino pair production at next-to-leading order and next-to-leading logarithmic accuracy. The updated cross sections have been computed for experimentally relevant higgsino and gaugino search channels at the ongoing Run II of the LHC. A factorisation method is applied to exploit the smaller PDF uncertainty of the global PDF sets and to avoid complications arising in the refitting of threshold-resummation improved PDF repl"},"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":"1805.11322","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-05-29T09:26:46Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"c094bb25105d7c59fbd61c0639de8e56163cc88a391a68c445d945ecd1607fb9","abstract_canon_sha256":"74818861a407f3f11e9a025f794fce14f34a59e2e0d6d514b22a57424f09dae6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:05:30.995161Z","signature_b64":"LShjxQ335qGNJjgWEXPTih27a9ChTH9TI7IBEhqD7afmkpKgXUFZqghwMmokl0+pbSfddfOeCVFZrZlZ+hxHCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6c996729422813340e86fec8caabac8f778fd4fd66e59797e82eaef8201de60b","last_reissued_at":"2026-05-18T00:05:30.994755Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:05:30.994755Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Neutralino/chargino pair production at NLO+NLL with resummation-improved PDFs for LHC Run II","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"J. Fiaschi, M. Klasen","submitted_at":"2018-05-29T09:26:46Z","abstract_excerpt":"We make use of recently released parton density functions (PDFs) with threshold-resummation improvement to consistently calculate theoretical predictions for neutralino and chargino pair production at next-to-leading order and next-to-leading logarithmic accuracy. The updated cross sections have been computed for experimentally relevant higgsino and gaugino search channels at the ongoing Run II of the LHC. A factorisation method is applied to exploit the smaller PDF uncertainty of the global PDF sets and to avoid complications arising in the refitting of threshold-resummation improved PDF repl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.11322","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":""},"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":"1805.11322","created_at":"2026-05-18T00:05:30.994822+00:00"},{"alias_kind":"arxiv_version","alias_value":"1805.11322v2","created_at":"2026-05-18T00:05:30.994822+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.11322","created_at":"2026-05-18T00:05:30.994822+00:00"},{"alias_kind":"pith_short_12","alias_value":"NSMWOKKCFAJT","created_at":"2026-05-18T12:32:40.477152+00:00"},{"alias_kind":"pith_short_16","alias_value":"NSMWOKKCFAJTIDUG","created_at":"2026-05-18T12:32:40.477152+00:00"},{"alias_kind":"pith_short_8","alias_value":"NSMWOKKC","created_at":"2026-05-18T12:32:40.477152+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2511.21240","citing_title":"Search for signatures of electroweakinos with photons, jets, and large missing transverse momentum in $\\sqrt{s}=13$ TeV pp collisions with the ATLAS detector","ref_index":48,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NSMWOKKCFAJTIDUG73EMVK5MR5","json":"https://pith.science/pith/NSMWOKKCFAJTIDUG73EMVK5MR5.json","graph_json":"https://pith.science/api/pith-number/NSMWOKKCFAJTIDUG73EMVK5MR5/graph.json","events_json":"https://pith.science/api/pith-number/NSMWOKKCFAJTIDUG73EMVK5MR5/events.json","paper":"https://pith.science/paper/NSMWOKKC"},"agent_actions":{"view_html":"https://pith.science/pith/NSMWOKKCFAJTIDUG73EMVK5MR5","download_json":"https://pith.science/pith/NSMWOKKCFAJTIDUG73EMVK5MR5.json","view_paper":"https://pith.science/paper/NSMWOKKC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1805.11322&json=true","fetch_graph":"https://pith.science/api/pith-number/NSMWOKKCFAJTIDUG73EMVK5MR5/graph.json","fetch_events":"https://pith.science/api/pith-number/NSMWOKKCFAJTIDUG73EMVK5MR5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NSMWOKKCFAJTIDUG73EMVK5MR5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NSMWOKKCFAJTIDUG73EMVK5MR5/action/storage_attestation","attest_author":"https://pith.science/pith/NSMWOKKCFAJTIDUG73EMVK5MR5/action/author_attestation","sign_citation":"https://pith.science/pith/NSMWOKKCFAJTIDUG73EMVK5MR5/action/citation_signature","submit_replication":"https://pith.science/pith/NSMWOKKCFAJTIDUG73EMVK5MR5/action/replication_record"}},"created_at":"2026-05-18T00:05:30.994822+00:00","updated_at":"2026-05-18T00:05:30.994822+00:00"}