{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:45E62QQVJPUKL5J3FL322U75FS","short_pith_number":"pith:45E62QQV","schema_version":"1.0","canonical_sha256":"e749ed42154be8a5f53b2af7ad53fd2c8a4acd101f771b2fdb0f1972470856c7","source":{"kind":"arxiv","id":"1512.03433","version":2},"attestation_state":"computed","paper":{"title":"2, 84, 30, 993, 560, 15456, 11962, 261485, ...: Higher dimension operators in the SM EFT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Brian Henning, Hitoshi Murayama, Tom Melia, Xiaochuan Lu","submitted_at":"2015-12-10T21:00:09Z","abstract_excerpt":"In a companion paper, we show that operator bases for general effective field theories are controlled by the conformal algebra. Equations of motion and integration by parts identities can be systematically treated by organizing operators into irreducible representations of the conformal group. In the present work, we use this result to study the standard model effective field theory (SM EFT), determining the content and number of higher dimension operators up to dimension 12, for an arbitrary number of fermion generations. We find additional operators to those that have appeared in the literat"},"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":"1512.03433","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-12-10T21:00:09Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"c0950aaa522e972763e890c9d93eee7512173a6a554d5d8f512f69a97bdb1026","abstract_canon_sha256":"38a0b207347c2aadb012200f4c8e71bc224d19da2acd0f2524f4fa21069c9415"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T23:59:13.997616Z","signature_b64":"cR4dcYKq65Z3d3AqHAaCdXWEFonmHWm+mYEibVgGL7n3vnwsvPezoDnXwEpC8rPK3PQZXlmLW0rErFk8Tl+BDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e749ed42154be8a5f53b2af7ad53fd2c8a4acd101f771b2fdb0f1972470856c7","last_reissued_at":"2026-07-04T23:59:13.997163Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T23:59:13.997163Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"2, 84, 30, 993, 560, 15456, 11962, 261485, ...: Higher dimension operators in the SM EFT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Brian Henning, Hitoshi Murayama, Tom Melia, Xiaochuan Lu","submitted_at":"2015-12-10T21:00:09Z","abstract_excerpt":"In a companion paper, we show that operator bases for general effective field theories are controlled by the conformal algebra. Equations of motion and integration by parts identities can be systematically treated by organizing operators into irreducible representations of the conformal group. In the present work, we use this result to study the standard model effective field theory (SM EFT), determining the content and number of higher dimension operators up to dimension 12, for an arbitrary number of fermion generations. We find additional operators to those that have appeared in the literat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.03433","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1512.03433/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":"1512.03433","created_at":"2026-07-04T23:59:13.997229+00:00"},{"alias_kind":"arxiv_version","alias_value":"1512.03433v2","created_at":"2026-07-04T23:59:13.997229+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.03433","created_at":"2026-07-04T23:59:13.997229+00:00"},{"alias_kind":"pith_short_12","alias_value":"45E62QQVJPUK","created_at":"2026-07-04T23:59:13.997229+00:00"},{"alias_kind":"pith_short_16","alias_value":"45E62QQVJPUKL5J3","created_at":"2026-07-04T23:59:13.997229+00:00"},{"alias_kind":"pith_short_8","alias_value":"45E62QQV","created_at":"2026-07-04T23:59:13.997229+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":9,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.26097","citing_title":"Positron-Emitting and Electron-Capturing Double-Beta Processes in the Standard Model and Beyond","ref_index":49,"is_internal_anchor":false},{"citing_arxiv_id":"1906.10631","citing_title":"Towards global fits in EFT's and New Physics implications","ref_index":5,"is_internal_anchor":false},{"citing_arxiv_id":"1907.07605","citing_title":"Complete One-Loop Renormalization of the Higgs-Electroweak Chiral Lagrangian","ref_index":7,"is_internal_anchor":false},{"citing_arxiv_id":"2511.23410","citing_title":"The Art of Counting: a reappraisal of the HEFT expansion","ref_index":73,"is_internal_anchor":false},{"citing_arxiv_id":"2601.21040","citing_title":"Constraining dimension-6 SMEFT with higher-order predictions for $p p \\to t W$","ref_index":14,"is_internal_anchor":false},{"citing_arxiv_id":"2604.25771","citing_title":"Covariant Construction of Generalized Form Factors","ref_index":59,"is_internal_anchor":false},{"citing_arxiv_id":"2604.25134","citing_title":"Basis for non-derivative baryon-number-violating operators","ref_index":24,"is_internal_anchor":false},{"citing_arxiv_id":"2604.22608","citing_title":"Recent Developments in SMEFT: Theory, Tools, and Phenomenology","ref_index":37,"is_internal_anchor":false},{"citing_arxiv_id":"2605.02878","citing_title":"Finite-temperature operator basis on $\\mathbb{R}^3 \\times S^1$ for SMEFT","ref_index":45,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/45E62QQVJPUKL5J3FL322U75FS","json":"https://pith.science/pith/45E62QQVJPUKL5J3FL322U75FS.json","graph_json":"https://pith.science/api/pith-number/45E62QQVJPUKL5J3FL322U75FS/graph.json","events_json":"https://pith.science/api/pith-number/45E62QQVJPUKL5J3FL322U75FS/events.json","paper":"https://pith.science/paper/45E62QQV"},"agent_actions":{"view_html":"https://pith.science/pith/45E62QQVJPUKL5J3FL322U75FS","download_json":"https://pith.science/pith/45E62QQVJPUKL5J3FL322U75FS.json","view_paper":"https://pith.science/paper/45E62QQV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1512.03433&json=true","fetch_graph":"https://pith.science/api/pith-number/45E62QQVJPUKL5J3FL322U75FS/graph.json","fetch_events":"https://pith.science/api/pith-number/45E62QQVJPUKL5J3FL322U75FS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/45E62QQVJPUKL5J3FL322U75FS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/45E62QQVJPUKL5J3FL322U75FS/action/storage_attestation","attest_author":"https://pith.science/pith/45E62QQVJPUKL5J3FL322U75FS/action/author_attestation","sign_citation":"https://pith.science/pith/45E62QQVJPUKL5J3FL322U75FS/action/citation_signature","submit_replication":"https://pith.science/pith/45E62QQVJPUKL5J3FL322U75FS/action/replication_record"}},"created_at":"2026-07-04T23:59:13.997229+00:00","updated_at":"2026-07-04T23:59:13.997229+00:00"}