{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:4NTIJBJBWUSGA562L5F5VW3LY5","short_pith_number":"pith:4NTIJBJB","schema_version":"1.0","canonical_sha256":"e366848521b5246077da5f4bdadb6bc75eb57acb83fbbe4c15260db294d77836","source":{"kind":"arxiv","id":"1308.2627","version":4},"attestation_state":"computed","paper":{"title":"Renormalization Group Evolution of the Standard Model Dimension Six Operators I: Formalism and lambda Dependence","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Aneesh V.Manohar, Elizabeth E. Jenkins, Michael Trott","submitted_at":"2013-08-12T17:21:12Z","abstract_excerpt":"We calculate the order \\lambda, \\lambda^2 and \\lambda y^2 terms of the 59 x 59 one-loop anomalous dimension matrix of dimension-six operators, where \\lambda and y are the Standard Model Higgs self-coupling and a generic Yukawa coupling, respectively. The dimension-six operators modify the running of the Standard Model parameters themselves, and we compute the complete one-loop result for this. We discuss how there is mixing between operators for which no direct one-particle-irreducible diagram exists, due to operator replacements by the equations of motion."},"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":"1308.2627","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-08-12T17:21:12Z","cross_cats_sorted":[],"title_canon_sha256":"8d14b8164158d35f5c9b254fd63e56525ca2d6ad95e939dc64c2cc0f36145dfb","abstract_canon_sha256":"9eb467c8c8bd56897daf61314a6ca688d79439d5087de58b82e408ecbf17927d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:19:22.582803Z","signature_b64":"YEOY2LUToliKO/7GWjpnZ7n6Ic4oeBJWCRATJ4Ssq44VMPhHD46t0yDOYLv4rf0st5Sb648mDBl1ZsTPTqWRCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e366848521b5246077da5f4bdadb6bc75eb57acb83fbbe4c15260db294d77836","last_reissued_at":"2026-07-05T01:19:22.582264Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:19:22.582264Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Renormalization Group Evolution of the Standard Model Dimension Six Operators I: Formalism and lambda Dependence","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Aneesh V.Manohar, Elizabeth E. Jenkins, Michael Trott","submitted_at":"2013-08-12T17:21:12Z","abstract_excerpt":"We calculate the order \\lambda, \\lambda^2 and \\lambda y^2 terms of the 59 x 59 one-loop anomalous dimension matrix of dimension-six operators, where \\lambda and y are the Standard Model Higgs self-coupling and a generic Yukawa coupling, respectively. The dimension-six operators modify the running of the Standard Model parameters themselves, and we compute the complete one-loop result for this. We discuss how there is mixing between operators for which no direct one-particle-irreducible diagram exists, due to operator replacements by the equations of motion."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1308.2627","kind":"arxiv","version":4},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1308.2627/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"1308.2627","created_at":"2026-07-05T01:19:22.582326+00:00"},{"alias_kind":"arxiv_version","alias_value":"1308.2627v4","created_at":"2026-07-05T01:19:22.582326+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1308.2627","created_at":"2026-07-05T01:19:22.582326+00:00"},{"alias_kind":"pith_short_12","alias_value":"4NTIJBJBWUSG","created_at":"2026-07-05T01:19:22.582326+00:00"},{"alias_kind":"pith_short_16","alias_value":"4NTIJBJBWUSGA562","created_at":"2026-07-05T01:19:22.582326+00:00"},{"alias_kind":"pith_short_8","alias_value":"4NTIJBJB","created_at":"2026-07-05T01:19:22.582326+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":23,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.07811","citing_title":"Impact of QED Radiation on SMEFT Constraints in Deep Inelastic Scattering","ref_index":14,"is_internal_anchor":true},{"citing_arxiv_id":"2606.26097","citing_title":"Positron-Emitting and Electron-Capturing Double-Beta Processes in the Standard Model and Beyond","ref_index":62,"is_internal_anchor":false},{"citing_arxiv_id":"2606.19202","citing_title":"Renormalization of the SMEFT to Dimension Eight: Fermionic Interactions II","ref_index":29,"is_internal_anchor":false},{"citing_arxiv_id":"2606.17132","citing_title":"Are neutrinos Majorana? Fixed-target and high-energy astrophysical searches decide","ref_index":15,"is_internal_anchor":false},{"citing_arxiv_id":"2606.12312","citing_title":"Sensitivity to top-quark couplings in diboson production at lepton colliders","ref_index":43,"is_internal_anchor":false},{"citing_arxiv_id":"2606.09596","citing_title":"Lifting Effective-Field-Theory Degeneracies in Semileptonic Heavy-Baryon Decays","ref_index":26,"is_internal_anchor":false},{"citing_arxiv_id":"2606.07232","citing_title":"Current and future constraints on heavy New Physics from $\\tau$ weak dipole moments","ref_index":23,"is_internal_anchor":false},{"citing_arxiv_id":"2607.00136","citing_title":"The left-cut for partial waves in terms of physical amplitudes","ref_index":4,"is_internal_anchor":false},{"citing_arxiv_id":"2606.02709","citing_title":"Anatomy and Phenomenology of Minimal Flavor Deconstruction in the Lepton Sector","ref_index":82,"is_internal_anchor":false},{"citing_arxiv_id":"2605.11747","citing_title":"SMEFT everywhere: a NLO study of $\\boldsymbol{pp \\to t\\bar{t}H}$ with decaying tops","ref_index":26,"is_internal_anchor":false},{"citing_arxiv_id":"2605.27525","citing_title":"Hunting New Animalcula with Flavour Changing Processes","ref_index":25,"is_internal_anchor":false},{"citing_arxiv_id":"1906.10631","citing_title":"Towards global fits in EFT's and New Physics implications","ref_index":12,"is_internal_anchor":false},{"citing_arxiv_id":"1907.07605","citing_title":"Complete One-Loop Renormalization of the Higgs-Electroweak Chiral Lagrangian","ref_index":12,"is_internal_anchor":false},{"citing_arxiv_id":"2605.21594","citing_title":"Exploring the SMEFT landscape: Bayesian Model Selection for indirect discovery","ref_index":37,"is_internal_anchor":false},{"citing_arxiv_id":"2605.21721","citing_title":"The Higgs-top-$Z$ mass coincidence relation after NNLO matching","ref_index":16,"is_internal_anchor":false},{"citing_arxiv_id":"2601.18237","citing_title":"Revisiting $\\mu$-$e$ conversion in $R$-parity violating SUSY","ref_index":58,"is_internal_anchor":false},{"citing_arxiv_id":"2605.11747","citing_title":"SMEFT everywhere: a NLO study of $\\boldsymbol{pp \\to t\\bar{t}H}$ with decaying tops","ref_index":26,"is_internal_anchor":false},{"citing_arxiv_id":"2604.26817","citing_title":"When Two Loops Matter: Electroweak Precision in the SMEFT","ref_index":27,"is_internal_anchor":false},{"citing_arxiv_id":"2605.08433","citing_title":"Electroweak Restoration: SMEFT and HEFT","ref_index":16,"is_internal_anchor":false},{"citing_arxiv_id":"2604.22608","citing_title":"Recent Developments in SMEFT: Theory, Tools, and Phenomenology","ref_index":26,"is_internal_anchor":false},{"citing_arxiv_id":"2604.14091","citing_title":"Exploring new resonances with direct top flavor changing interactions","ref_index":21,"is_internal_anchor":false},{"citing_arxiv_id":"2604.14281","citing_title":"Probing $\\tau$ lepton dipole moments at future Lepton Colliders","ref_index":63,"is_internal_anchor":false},{"citing_arxiv_id":"2604.16599","citing_title":"The effect of the two-loop SMEFT RGEs at future colliders","ref_index":1,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4NTIJBJBWUSGA562L5F5VW3LY5","json":"https://pith.science/pith/4NTIJBJBWUSGA562L5F5VW3LY5.json","graph_json":"https://pith.science/api/pith-number/4NTIJBJBWUSGA562L5F5VW3LY5/graph.json","events_json":"https://pith.science/api/pith-number/4NTIJBJBWUSGA562L5F5VW3LY5/events.json","paper":"https://pith.science/paper/4NTIJBJB"},"agent_actions":{"view_html":"https://pith.science/pith/4NTIJBJBWUSGA562L5F5VW3LY5","download_json":"https://pith.science/pith/4NTIJBJBWUSGA562L5F5VW3LY5.json","view_paper":"https://pith.science/paper/4NTIJBJB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1308.2627&json=true","fetch_graph":"https://pith.science/api/pith-number/4NTIJBJBWUSGA562L5F5VW3LY5/graph.json","fetch_events":"https://pith.science/api/pith-number/4NTIJBJBWUSGA562L5F5VW3LY5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4NTIJBJBWUSGA562L5F5VW3LY5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4NTIJBJBWUSGA562L5F5VW3LY5/action/storage_attestation","attest_author":"https://pith.science/pith/4NTIJBJBWUSGA562L5F5VW3LY5/action/author_attestation","sign_citation":"https://pith.science/pith/4NTIJBJBWUSGA562L5F5VW3LY5/action/citation_signature","submit_replication":"https://pith.science/pith/4NTIJBJBWUSGA562L5F5VW3LY5/action/replication_record"}},"created_at":"2026-07-05T01:19:22.582326+00:00","updated_at":"2026-07-05T01:19:22.582326+00:00"}