{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:XQLBV27NBP3ZFKFXU2SHPOCMT3","short_pith_number":"pith:XQLBV27N","schema_version":"1.0","canonical_sha256":"bc161aebed0bf792a8b7a6a477b84c9eec5e3bc7ef616082adec838d90ea0098","source":{"kind":"arxiv","id":"1001.1307","version":2},"attestation_state":"computed","paper":{"title":"A proposal for a standard interface between Monte Carlo tools and one-loop programs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Denner, A. Lazopoulos, C. Oleari, D. Maitre, F. Boudjema, F. Krauss, F. Maltoni, G. Dissertori, G. Heinrich, G. Passarino, G. Zanderighi, J. Archibald, J. Huston, J. Winter, M. Huber, N. Greiner, N. Kauer, P. Skands, R. Frederix, R. Pittau, S. Dittmaier, S. Hoche, S. Pozzorini, S. Schumann, T. Binoth, T. Gleisberg, T. Reiter, W. Giele","submitted_at":"2010-01-08T15:48:17Z","abstract_excerpt":"Many highly developed Monte Carlo tools for the evaluation of cross sections based on tree matrix elements exist and are used by experimental collaborations in high energy physics. As the evaluation of one-loop matrix elements has recently been undergoing enormous progress, the combination of one-loop matrix elements with existing Monte Carlo tools is on the horizon. This would lead to phenomenological predictions at the next-to-leading order level. This note summarises the discussion of the next-to-leading order multi-leg (NLM) working group on this issue which has been taking place during th"},"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":"1001.1307","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-01-08T15:48:17Z","cross_cats_sorted":[],"title_canon_sha256":"9a6ad8d5e2b0645779012f201da03bf373b689df6326b060d0cdb42ccd459903","abstract_canon_sha256":"101b71a59be9ffa753e75f773fef729a965b64d4a9ce9ccead7e9f2e4753d708"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:33:50.073515Z","signature_b64":"DJT5LTyVai8pArM0uQHcgHn0yfVltrTzA8Ud41tSXiHM1mlndCiTcB/GPpbtndnZda0/USXuCfIZNxg7WzAsCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bc161aebed0bf792a8b7a6a477b84c9eec5e3bc7ef616082adec838d90ea0098","last_reissued_at":"2026-05-18T02:33:50.073071Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:33:50.073071Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A proposal for a standard interface between Monte Carlo tools and one-loop programs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Denner, A. Lazopoulos, C. Oleari, D. Maitre, F. Boudjema, F. Krauss, F. Maltoni, G. Dissertori, G. Heinrich, G. Passarino, G. Zanderighi, J. Archibald, J. Huston, J. Winter, M. Huber, N. Greiner, N. Kauer, P. Skands, R. Frederix, R. Pittau, S. Dittmaier, S. Hoche, S. Pozzorini, S. Schumann, T. Binoth, T. Gleisberg, T. Reiter, W. Giele","submitted_at":"2010-01-08T15:48:17Z","abstract_excerpt":"Many highly developed Monte Carlo tools for the evaluation of cross sections based on tree matrix elements exist and are used by experimental collaborations in high energy physics. As the evaluation of one-loop matrix elements has recently been undergoing enormous progress, the combination of one-loop matrix elements with existing Monte Carlo tools is on the horizon. This would lead to phenomenological predictions at the next-to-leading order level. This note summarises the discussion of the next-to-leading order multi-leg (NLM) working group on this issue which has been taking place during th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1001.1307","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":"1001.1307","created_at":"2026-05-18T02:33:50.073141+00:00"},{"alias_kind":"arxiv_version","alias_value":"1001.1307v2","created_at":"2026-05-18T02:33:50.073141+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1001.1307","created_at":"2026-05-18T02:33:50.073141+00:00"},{"alias_kind":"pith_short_12","alias_value":"XQLBV27NBP3Z","created_at":"2026-05-18T12:26:17.028572+00:00"},{"alias_kind":"pith_short_16","alias_value":"XQLBV27NBP3ZFKFX","created_at":"2026-05-18T12:26:17.028572+00:00"},{"alias_kind":"pith_short_8","alias_value":"XQLBV27N","created_at":"2026-05-18T12:26:17.028572+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1906.12310","citing_title":"Proposal for the validation of Monte Carlo implementations of the standard model effective field theory","ref_index":31,"is_internal_anchor":true},{"citing_arxiv_id":"1002.2581","citing_title":"A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX","ref_index":21,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XQLBV27NBP3ZFKFXU2SHPOCMT3","json":"https://pith.science/pith/XQLBV27NBP3ZFKFXU2SHPOCMT3.json","graph_json":"https://pith.science/api/pith-number/XQLBV27NBP3ZFKFXU2SHPOCMT3/graph.json","events_json":"https://pith.science/api/pith-number/XQLBV27NBP3ZFKFXU2SHPOCMT3/events.json","paper":"https://pith.science/paper/XQLBV27N"},"agent_actions":{"view_html":"https://pith.science/pith/XQLBV27NBP3ZFKFXU2SHPOCMT3","download_json":"https://pith.science/pith/XQLBV27NBP3ZFKFXU2SHPOCMT3.json","view_paper":"https://pith.science/paper/XQLBV27N","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1001.1307&json=true","fetch_graph":"https://pith.science/api/pith-number/XQLBV27NBP3ZFKFXU2SHPOCMT3/graph.json","fetch_events":"https://pith.science/api/pith-number/XQLBV27NBP3ZFKFXU2SHPOCMT3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XQLBV27NBP3ZFKFXU2SHPOCMT3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XQLBV27NBP3ZFKFXU2SHPOCMT3/action/storage_attestation","attest_author":"https://pith.science/pith/XQLBV27NBP3ZFKFXU2SHPOCMT3/action/author_attestation","sign_citation":"https://pith.science/pith/XQLBV27NBP3ZFKFXU2SHPOCMT3/action/citation_signature","submit_replication":"https://pith.science/pith/XQLBV27NBP3ZFKFXU2SHPOCMT3/action/replication_record"}},"created_at":"2026-05-18T02:33:50.073141+00:00","updated_at":"2026-05-18T02:33:50.073141+00:00"}