{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:HRZU5U5ID3VMUATBEIPEKR62UP","short_pith_number":"pith:HRZU5U5I","schema_version":"1.0","canonical_sha256":"3c734ed3a81eeaca0261221e4547daa3f8039adadf572680f086e2d912e3c2c0","source":{"kind":"arxiv","id":"1007.3492","version":1},"attestation_state":"computed","paper":{"title":"MCFM for the Tevatron and the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"John M Campbell, R. K. Ellis","submitted_at":"2010-07-20T19:50:43Z","abstract_excerpt":"A summary is given of the current status of the next-to-leading order (NLO) parton-level integrator MCFM. Some details are given about the Higgs + 2-jet process and the production and decay of $t \\bar{t}$, both of which have recently been added to the code. Using MCFM, comparisons between the Tevatron running at $\\sqrt{s}=2$~TeV and the LHC running at $\\sqrt{s}=7$~TeV are made for standard model process including the production of Higgs bosons. The case for running the Tevatron until 16fb$^{-1}$ are accumulated by both detectors is sketched."},"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":"1007.3492","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-07-20T19:50:43Z","cross_cats_sorted":[],"title_canon_sha256":"bc75828cf9941cc363c13d054e0ea33a5c2f56a5f220ed8ceb40556d1c7741aa","abstract_canon_sha256":"029d670b0141f6dfe9ecb0eb4d43025a3c62b7b48b09634cd5a2f4b5f470d218"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:33:39.167677Z","signature_b64":"pMagWpQeWdNaKF1g4+p5AprcJi87YyVBYrAjXuhfn188Ie/rPT406LJRitL0bSz2Fv1e0LgB3NDDCPMcrkhrCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3c734ed3a81eeaca0261221e4547daa3f8039adadf572680f086e2d912e3c2c0","last_reissued_at":"2026-05-18T04:33:39.166930Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:33:39.166930Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"MCFM for the Tevatron and the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"John M Campbell, R. K. Ellis","submitted_at":"2010-07-20T19:50:43Z","abstract_excerpt":"A summary is given of the current status of the next-to-leading order (NLO) parton-level integrator MCFM. Some details are given about the Higgs + 2-jet process and the production and decay of $t \\bar{t}$, both of which have recently been added to the code. Using MCFM, comparisons between the Tevatron running at $\\sqrt{s}=2$~TeV and the LHC running at $\\sqrt{s}=7$~TeV are made for standard model process including the production of Higgs bosons. The case for running the Tevatron until 16fb$^{-1}$ are accumulated by both detectors is sketched."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1007.3492","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":"1007.3492","created_at":"2026-05-18T04:33:39.167010+00:00"},{"alias_kind":"arxiv_version","alias_value":"1007.3492v1","created_at":"2026-05-18T04:33:39.167010+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1007.3492","created_at":"2026-05-18T04:33:39.167010+00:00"},{"alias_kind":"pith_short_12","alias_value":"HRZU5U5ID3VM","created_at":"2026-05-18T12:26:07.630475+00:00"},{"alias_kind":"pith_short_16","alias_value":"HRZU5U5ID3VMUATB","created_at":"2026-05-18T12:26:07.630475+00:00"},{"alias_kind":"pith_short_8","alias_value":"HRZU5U5I","created_at":"2026-05-18T12:26:07.630475+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":5,"sample":[{"citing_arxiv_id":"2504.02958","citing_title":"Combined effective field theory interpretation of Higgs boson, electroweak vector boson, top quark, and multi-jet measurements","ref_index":70,"is_internal_anchor":true},{"citing_arxiv_id":"1912.10053","citing_title":"New CTEQ global analysis of quantum chromodynamics with high-precision data from the LHC","ref_index":46,"is_internal_anchor":true},{"citing_arxiv_id":"2511.23091","citing_title":"Measurement of the top-quark mass using decays with a $J/\\psi$ meson at $\\sqrt{s}=$13 TeV with the ATLAS detector","ref_index":125,"is_internal_anchor":true},{"citing_arxiv_id":"2512.04959","citing_title":"Towards a Fully Automated Differential $\\text{NNLO}_\\text{EW}$ Generator for Lepton Colliders","ref_index":85,"is_internal_anchor":true},{"citing_arxiv_id":"2605.13614","citing_title":"Search for pair production of additional neutral scalars within the Inert Doublet Model in a final state with two electrons or two muons in proton-proton collisions at $\\sqrt{s}$ = 13 TeV and 13.6 TeV","ref_index":59,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HRZU5U5ID3VMUATBEIPEKR62UP","json":"https://pith.science/pith/HRZU5U5ID3VMUATBEIPEKR62UP.json","graph_json":"https://pith.science/api/pith-number/HRZU5U5ID3VMUATBEIPEKR62UP/graph.json","events_json":"https://pith.science/api/pith-number/HRZU5U5ID3VMUATBEIPEKR62UP/events.json","paper":"https://pith.science/paper/HRZU5U5I"},"agent_actions":{"view_html":"https://pith.science/pith/HRZU5U5ID3VMUATBEIPEKR62UP","download_json":"https://pith.science/pith/HRZU5U5ID3VMUATBEIPEKR62UP.json","view_paper":"https://pith.science/paper/HRZU5U5I","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1007.3492&json=true","fetch_graph":"https://pith.science/api/pith-number/HRZU5U5ID3VMUATBEIPEKR62UP/graph.json","fetch_events":"https://pith.science/api/pith-number/HRZU5U5ID3VMUATBEIPEKR62UP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HRZU5U5ID3VMUATBEIPEKR62UP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HRZU5U5ID3VMUATBEIPEKR62UP/action/storage_attestation","attest_author":"https://pith.science/pith/HRZU5U5ID3VMUATBEIPEKR62UP/action/author_attestation","sign_citation":"https://pith.science/pith/HRZU5U5ID3VMUATBEIPEKR62UP/action/citation_signature","submit_replication":"https://pith.science/pith/HRZU5U5ID3VMUATBEIPEKR62UP/action/replication_record"}},"created_at":"2026-05-18T04:33:39.167010+00:00","updated_at":"2026-05-18T04:33:39.167010+00:00"}