{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:T3ZMJIP7WGOGLJI5FQNFSXWD3H","short_pith_number":"pith:T3ZMJIP7","schema_version":"1.0","canonical_sha256":"9ef2c4a1ffb19c65a51d2c1a595ec3d9d45f4426c49d2ee19c72daf3cf282934","source":{"kind":"arxiv","id":"2309.16611","version":2},"attestation_state":"computed","paper":{"title":"Positivity restrictions on the mixing of dimension-eight SMEFT operators","license":"http://creativecommons.org/licenses/by-sa/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Mikael Chala, Xu Li","submitted_at":"2023-09-28T17:10:00Z","abstract_excerpt":"We discuss the structure of the mixing among dimension-eight operators in the SMEFT relying on the positivity of two-to-two forward scattering amplitudes. We uncover tens of new non-trivial zeros as well as hundreds of terms with definite sign in (a particular basis of) the corresponding anomalous dimension matrix. We highlight that our results are not immediately apparent from the Feynman diagrammatic perspective, nor from on-shell amplitude methods. As a byproduct of this work, we provide positivity bounds not previously derived in the literature, as well as explicit values of certain elemen"},"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":"2309.16611","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"hep-ph","submitted_at":"2023-09-28T17:10:00Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"82e5ddfab7e430c9b20f6a4cb09c7fbecc098b0cfdf91fde651ea03418862fe2","abstract_canon_sha256":"ac6640a03f750316452930464f4aa00c41e5763da4745a0458d53ff9cd573fb5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:40:57.556288Z","signature_b64":"6rhAJWZzPw5x3gtkZyTWZDHhuvMjy6LUwkT6+zjp83p6W58QtDMfcz8bLzfNJBPMCjeUymjFXU7DdSUZQK3aCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9ef2c4a1ffb19c65a51d2c1a595ec3d9d45f4426c49d2ee19c72daf3cf282934","last_reissued_at":"2026-07-05T07:40:57.555756Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:40:57.555756Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Positivity restrictions on the mixing of dimension-eight SMEFT operators","license":"http://creativecommons.org/licenses/by-sa/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Mikael Chala, Xu Li","submitted_at":"2023-09-28T17:10:00Z","abstract_excerpt":"We discuss the structure of the mixing among dimension-eight operators in the SMEFT relying on the positivity of two-to-two forward scattering amplitudes. We uncover tens of new non-trivial zeros as well as hundreds of terms with definite sign in (a particular basis of) the corresponding anomalous dimension matrix. We highlight that our results are not immediately apparent from the Feynman diagrammatic perspective, nor from on-shell amplitude methods. As a byproduct of this work, we provide positivity bounds not previously derived in the literature, as well as explicit values of certain elemen"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2309.16611","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/2309.16611/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":"2309.16611","created_at":"2026-07-05T07:40:57.555816+00:00"},{"alias_kind":"arxiv_version","alias_value":"2309.16611v2","created_at":"2026-07-05T07:40:57.555816+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2309.16611","created_at":"2026-07-05T07:40:57.555816+00:00"},{"alias_kind":"pith_short_12","alias_value":"T3ZMJIP7WGOG","created_at":"2026-07-05T07:40:57.555816+00:00"},{"alias_kind":"pith_short_16","alias_value":"T3ZMJIP7WGOGLJI5","created_at":"2026-07-05T07:40:57.555816+00:00"},{"alias_kind":"pith_short_8","alias_value":"T3ZMJIP7","created_at":"2026-07-05T07:40:57.555816+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.19202","citing_title":"Renormalization of the SMEFT to Dimension Eight: Fermionic Interactions II","ref_index":77,"is_internal_anchor":false},{"citing_arxiv_id":"2605.20319","citing_title":"The Equivalence Principle at High Energies Completes the Spectrum","ref_index":61,"is_internal_anchor":false},{"citing_arxiv_id":"2511.23411","citing_title":"Higgs pair production in gluon fusion to higher orders in Higgs Effective Field Theory","ref_index":70,"is_internal_anchor":false},{"citing_arxiv_id":"2604.00107","citing_title":"Full positivity bounds for anomalous quartic gauge couplings in SMEFT","ref_index":36,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/T3ZMJIP7WGOGLJI5FQNFSXWD3H","json":"https://pith.science/pith/T3ZMJIP7WGOGLJI5FQNFSXWD3H.json","graph_json":"https://pith.science/api/pith-number/T3ZMJIP7WGOGLJI5FQNFSXWD3H/graph.json","events_json":"https://pith.science/api/pith-number/T3ZMJIP7WGOGLJI5FQNFSXWD3H/events.json","paper":"https://pith.science/paper/T3ZMJIP7"},"agent_actions":{"view_html":"https://pith.science/pith/T3ZMJIP7WGOGLJI5FQNFSXWD3H","download_json":"https://pith.science/pith/T3ZMJIP7WGOGLJI5FQNFSXWD3H.json","view_paper":"https://pith.science/paper/T3ZMJIP7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2309.16611&json=true","fetch_graph":"https://pith.science/api/pith-number/T3ZMJIP7WGOGLJI5FQNFSXWD3H/graph.json","fetch_events":"https://pith.science/api/pith-number/T3ZMJIP7WGOGLJI5FQNFSXWD3H/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/T3ZMJIP7WGOGLJI5FQNFSXWD3H/action/timestamp_anchor","attest_storage":"https://pith.science/pith/T3ZMJIP7WGOGLJI5FQNFSXWD3H/action/storage_attestation","attest_author":"https://pith.science/pith/T3ZMJIP7WGOGLJI5FQNFSXWD3H/action/author_attestation","sign_citation":"https://pith.science/pith/T3ZMJIP7WGOGLJI5FQNFSXWD3H/action/citation_signature","submit_replication":"https://pith.science/pith/T3ZMJIP7WGOGLJI5FQNFSXWD3H/action/replication_record"}},"created_at":"2026-07-05T07:40:57.555816+00:00","updated_at":"2026-07-05T07:40:57.555816+00:00"}