{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:2PVPDTQM4YVBGZQS4PF424HXCO","short_pith_number":"pith:2PVPDTQM","schema_version":"1.0","canonical_sha256":"d3eaf1ce0ce62a136612e3cbcd70f713a519ea36b5d59fe25751523543f4b037","source":{"kind":"arxiv","id":"1004.2169","version":2},"attestation_state":"computed","paper":{"title":"Supersymmetric Higgs Production in Vector-Boson Fusion","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Heidi Rzehak, Michael Rauch, Tilman Plehn, Wolfgang Hollik","submitted_at":"2010-04-13T13:03:18Z","abstract_excerpt":"We present a full calculation of the supersymmetric NLO corrections to Higgs boson production via vector-boson fusion. The supersymmetric QCD corrections turn out to be significantly smaller than the electroweak ones. These higher-order corrections are an important ingredient to a precision analysis of the Higgs sector at the LHC."},"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":"1004.2169","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-04-13T13:03:18Z","cross_cats_sorted":[],"title_canon_sha256":"2ef3c279ffad5d6625ca3073bd4c31f46443b62fbeb007d4c2f02d9803a80dd0","abstract_canon_sha256":"f932385d2f437cd471ff1f982d28b099f1200e7018faa24e5f2756cb031efd06"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:33:34.387149Z","signature_b64":"m99BpffEsA2Rx4jZhpbBH+El7oNuF1IiEuvTCdAOJjCnA8WRF2Vb/usfQ87Fr2PENU1o9V1mc7cS11O/Vf47Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d3eaf1ce0ce62a136612e3cbcd70f713a519ea36b5d59fe25751523543f4b037","last_reissued_at":"2026-05-18T02:33:34.386781Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:33:34.386781Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Supersymmetric Higgs Production in Vector-Boson Fusion","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Heidi Rzehak, Michael Rauch, Tilman Plehn, Wolfgang Hollik","submitted_at":"2010-04-13T13:03:18Z","abstract_excerpt":"We present a full calculation of the supersymmetric NLO corrections to Higgs boson production via vector-boson fusion. The supersymmetric QCD corrections turn out to be significantly smaller than the electroweak ones. These higher-order corrections are an important ingredient to a precision analysis of the Higgs sector at the LHC."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1004.2169","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":"1004.2169","created_at":"2026-05-18T02:33:34.386839+00:00"},{"alias_kind":"arxiv_version","alias_value":"1004.2169v2","created_at":"2026-05-18T02:33:34.386839+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1004.2169","created_at":"2026-05-18T02:33:34.386839+00:00"},{"alias_kind":"pith_short_12","alias_value":"2PVPDTQM4YVB","created_at":"2026-05-18T12:26:03.138858+00:00"},{"alias_kind":"pith_short_16","alias_value":"2PVPDTQM4YVBGZQS","created_at":"2026-05-18T12:26:03.138858+00:00"},{"alias_kind":"pith_short_8","alias_value":"2PVPDTQM","created_at":"2026-05-18T12:26:03.138858+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/2PVPDTQM4YVBGZQS4PF424HXCO","json":"https://pith.science/pith/2PVPDTQM4YVBGZQS4PF424HXCO.json","graph_json":"https://pith.science/api/pith-number/2PVPDTQM4YVBGZQS4PF424HXCO/graph.json","events_json":"https://pith.science/api/pith-number/2PVPDTQM4YVBGZQS4PF424HXCO/events.json","paper":"https://pith.science/paper/2PVPDTQM"},"agent_actions":{"view_html":"https://pith.science/pith/2PVPDTQM4YVBGZQS4PF424HXCO","download_json":"https://pith.science/pith/2PVPDTQM4YVBGZQS4PF424HXCO.json","view_paper":"https://pith.science/paper/2PVPDTQM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1004.2169&json=true","fetch_graph":"https://pith.science/api/pith-number/2PVPDTQM4YVBGZQS4PF424HXCO/graph.json","fetch_events":"https://pith.science/api/pith-number/2PVPDTQM4YVBGZQS4PF424HXCO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2PVPDTQM4YVBGZQS4PF424HXCO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2PVPDTQM4YVBGZQS4PF424HXCO/action/storage_attestation","attest_author":"https://pith.science/pith/2PVPDTQM4YVBGZQS4PF424HXCO/action/author_attestation","sign_citation":"https://pith.science/pith/2PVPDTQM4YVBGZQS4PF424HXCO/action/citation_signature","submit_replication":"https://pith.science/pith/2PVPDTQM4YVBGZQS4PF424HXCO/action/replication_record"}},"created_at":"2026-05-18T02:33:34.386839+00:00","updated_at":"2026-05-18T02:33:34.386839+00:00"}