{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:G5LUHCZTBWSMOJ3H33QACDB5FQ","short_pith_number":"pith:G5LUHCZT","schema_version":"1.0","canonical_sha256":"3757438b330da4c72767dee0010c3d2c3110208bca81d2105c50016e23f6693e","source":{"kind":"arxiv","id":"1612.00868","version":3},"attestation_state":"computed","paper":{"title":"Symmetry and Action for Flavor-Kinematics Duality","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Chia-Hsien Shen, Clifford Cheung","submitted_at":"2016-12-02T21:36:52Z","abstract_excerpt":"We propose a new representation of the nonlinear sigma model that exhibits a manifest duality between flavor and kinematics. The fields couple exclusively through cubic Feynman vertices which also serve as the structure constants of an underlying kinematic algebra. The action is invariant under a combination of internal and spacetime symmetries whose conservation equations imply flavor-kinematics duality, ensuring that all Feynman diagrams satisfy kinematic Jacobi identities. Substituting flavor for kinematics, we derive a new cubic action for the special Galileon theory. In this picture, the "},"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":"1612.00868","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-12-02T21:36:52Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"3cac5bf05457c7f1da345ec1d031181fc7fab298eb84c17a58a8fae372f3aa92","abstract_canon_sha256":"6f629beeda2a5040a826a401cd8ab3955e648a767a8c048390d1cfb785764771"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:46:48.730134Z","signature_b64":"ESJevqjbCPkOVc+wF6JgnDU5dGMlvP3XJreWmrrgIMdVfcGsKajeNNZThcbz3ydU5mgNJQnwB7VWzVrgGVoQBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3757438b330da4c72767dee0010c3d2c3110208bca81d2105c50016e23f6693e","last_reissued_at":"2026-05-18T00:46:48.729484Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:46:48.729484Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Symmetry and Action for Flavor-Kinematics Duality","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Chia-Hsien Shen, Clifford Cheung","submitted_at":"2016-12-02T21:36:52Z","abstract_excerpt":"We propose a new representation of the nonlinear sigma model that exhibits a manifest duality between flavor and kinematics. The fields couple exclusively through cubic Feynman vertices which also serve as the structure constants of an underlying kinematic algebra. The action is invariant under a combination of internal and spacetime symmetries whose conservation equations imply flavor-kinematics duality, ensuring that all Feynman diagrams satisfy kinematic Jacobi identities. Substituting flavor for kinematics, we derive a new cubic action for the special Galileon theory. In this picture, the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1612.00868","kind":"arxiv","version":3},"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":"1612.00868","created_at":"2026-05-18T00:46:48.729575+00:00"},{"alias_kind":"arxiv_version","alias_value":"1612.00868v3","created_at":"2026-05-18T00:46:48.729575+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1612.00868","created_at":"2026-05-18T00:46:48.729575+00:00"},{"alias_kind":"pith_short_12","alias_value":"G5LUHCZTBWSM","created_at":"2026-05-18T12:30:15.759754+00:00"},{"alias_kind":"pith_short_16","alias_value":"G5LUHCZTBWSMOJ3H","created_at":"2026-05-18T12:30:15.759754+00:00"},{"alias_kind":"pith_short_8","alias_value":"G5LUHCZT","created_at":"2026-05-18T12:30:15.759754+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2605.21582","citing_title":"Multipositivity Constrains the Chiral Lagrangian","ref_index":22,"is_internal_anchor":true},{"citing_arxiv_id":"2510.25866","citing_title":"Hawking Radiation meets the Double Copy","ref_index":67,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/G5LUHCZTBWSMOJ3H33QACDB5FQ","json":"https://pith.science/pith/G5LUHCZTBWSMOJ3H33QACDB5FQ.json","graph_json":"https://pith.science/api/pith-number/G5LUHCZTBWSMOJ3H33QACDB5FQ/graph.json","events_json":"https://pith.science/api/pith-number/G5LUHCZTBWSMOJ3H33QACDB5FQ/events.json","paper":"https://pith.science/paper/G5LUHCZT"},"agent_actions":{"view_html":"https://pith.science/pith/G5LUHCZTBWSMOJ3H33QACDB5FQ","download_json":"https://pith.science/pith/G5LUHCZTBWSMOJ3H33QACDB5FQ.json","view_paper":"https://pith.science/paper/G5LUHCZT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1612.00868&json=true","fetch_graph":"https://pith.science/api/pith-number/G5LUHCZTBWSMOJ3H33QACDB5FQ/graph.json","fetch_events":"https://pith.science/api/pith-number/G5LUHCZTBWSMOJ3H33QACDB5FQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/G5LUHCZTBWSMOJ3H33QACDB5FQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/G5LUHCZTBWSMOJ3H33QACDB5FQ/action/storage_attestation","attest_author":"https://pith.science/pith/G5LUHCZTBWSMOJ3H33QACDB5FQ/action/author_attestation","sign_citation":"https://pith.science/pith/G5LUHCZTBWSMOJ3H33QACDB5FQ/action/citation_signature","submit_replication":"https://pith.science/pith/G5LUHCZTBWSMOJ3H33QACDB5FQ/action/replication_record"}},"created_at":"2026-05-18T00:46:48.729575+00:00","updated_at":"2026-05-18T00:46:48.729575+00:00"}