{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:A5G5GAJ7DMCZDPVAMNFAYYAUOP","short_pith_number":"pith:A5G5GAJ7","schema_version":"1.0","canonical_sha256":"074dd3013f1b0591bea0634a0c601473d25b810e2951eb7819593f6a25e28d05","source":{"kind":"arxiv","id":"1309.3741","version":1},"attestation_state":"computed","paper":{"title":"GoSam applications for automated NLO calculations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"E.Mirabella, F.Tramontano, G.Cullen, G.Heinrich, G.Luisoni, G.Ossola, H.van Deurzen, J.F. von Soden-Fraunhofen, J.Reichel, J.Schlenk, N.Greiner, P.Mastrolia, T.Peraro","submitted_at":"2013-09-15T09:53:20Z","abstract_excerpt":"We present applications of the program GoSam for the automated calculation of one-loop amplitudes. Results for NLO QCD corrections to beyond the Standard Model processes as well as Higgs plus up to three-jet production in gluon fusion are shown. We also discuss some new features of the program."},"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":"1309.3741","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-09-15T09:53:20Z","cross_cats_sorted":[],"title_canon_sha256":"cf9e2dd2c3b8be712ce63b6a7fca21ff063c942d7dd218c7b13af58a84d6b90e","abstract_canon_sha256":"d0e84cc2364c914013bfd0a20c2403bd4ff88f3653861b8358c7f714b821faf7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:47:41.702361Z","signature_b64":"1DX9s52MlC6bKRtEqFQoa5dJeGyqJMbBHFfUPfApIoY9rchX/ZvwyCC5KvFKN1TfN0+QDF3JQsQPOYbUukLuDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"074dd3013f1b0591bea0634a0c601473d25b810e2951eb7819593f6a25e28d05","last_reissued_at":"2026-05-18T01:47:41.701845Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:47:41.701845Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"GoSam applications for automated NLO calculations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"E.Mirabella, F.Tramontano, G.Cullen, G.Heinrich, G.Luisoni, G.Ossola, H.van Deurzen, J.F. von Soden-Fraunhofen, J.Reichel, J.Schlenk, N.Greiner, P.Mastrolia, T.Peraro","submitted_at":"2013-09-15T09:53:20Z","abstract_excerpt":"We present applications of the program GoSam for the automated calculation of one-loop amplitudes. Results for NLO QCD corrections to beyond the Standard Model processes as well as Higgs plus up to three-jet production in gluon fusion are shown. We also discuss some new features of the program."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1309.3741","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":""},"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":"1309.3741","created_at":"2026-05-18T01:47:41.701922+00:00"},{"alias_kind":"arxiv_version","alias_value":"1309.3741v1","created_at":"2026-05-18T01:47:41.701922+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1309.3741","created_at":"2026-05-18T01:47:41.701922+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/A5G5GAJ7DMCZDPVAMNFAYYAUOP","json":"https://pith.science/pith/A5G5GAJ7DMCZDPVAMNFAYYAUOP.json","graph_json":"https://pith.science/api/pith-number/A5G5GAJ7DMCZDPVAMNFAYYAUOP/graph.json","events_json":"https://pith.science/api/pith-number/A5G5GAJ7DMCZDPVAMNFAYYAUOP/events.json","paper":"https://pith.science/paper/A5G5GAJ7"},"agent_actions":{"view_html":"https://pith.science/pith/A5G5GAJ7DMCZDPVAMNFAYYAUOP","download_json":"https://pith.science/pith/A5G5GAJ7DMCZDPVAMNFAYYAUOP.json","view_paper":"https://pith.science/paper/A5G5GAJ7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1309.3741&json=true","fetch_graph":"https://pith.science/api/pith-number/A5G5GAJ7DMCZDPVAMNFAYYAUOP/graph.json","fetch_events":"https://pith.science/api/pith-number/A5G5GAJ7DMCZDPVAMNFAYYAUOP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/A5G5GAJ7DMCZDPVAMNFAYYAUOP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/A5G5GAJ7DMCZDPVAMNFAYYAUOP/action/storage_attestation","attest_author":"https://pith.science/pith/A5G5GAJ7DMCZDPVAMNFAYYAUOP/action/author_attestation","sign_citation":"https://pith.science/pith/A5G5GAJ7DMCZDPVAMNFAYYAUOP/action/citation_signature","submit_replication":"https://pith.science/pith/A5G5GAJ7DMCZDPVAMNFAYYAUOP/action/replication_record"}},"created_at":"2026-05-18T01:47:41.701922+00:00","updated_at":"2026-05-18T01:47:41.701922+00:00"}