{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:CITMRU5TESW7RSCYVTB2RHLNEF","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"ab443322a9481327b4cde12267df558d2598e2802ef79d56f0305a3076417bc7","cross_cats_sorted":["hep-ph","physics.class-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-10-27T09:59:09Z","title_canon_sha256":"d03f12eacf366cbf2b8863f4dafd759f21ddc7d20518371b0f4bb0fba8eb687a"},"schema_version":"1.0","source":{"id":"1910.12224","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1910.12224","created_at":"2026-07-05T00:38:46Z"},{"alias_kind":"arxiv_version","alias_value":"1910.12224v1","created_at":"2026-07-05T00:38:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1910.12224","created_at":"2026-07-05T00:38:46Z"},{"alias_kind":"pith_short_12","alias_value":"CITMRU5TESW7","created_at":"2026-07-05T00:38:46Z"},{"alias_kind":"pith_short_16","alias_value":"CITMRU5TESW7RSCY","created_at":"2026-07-05T00:38:46Z"},{"alias_kind":"pith_short_8","alias_value":"CITMRU5T","created_at":"2026-07-05T00:38:46Z"}],"graph_snapshots":[{"event_id":"sha256:7746570fc914d6d0ccbaf638d751a9f09c11ad3d685fd925ba15bf13ebb8c3cd","target":"graph","created_at":"2026-07-05T00:38:46Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/1910.12224/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Local symmetry transformations play an important role for establishing the existence and form of a conserved (Noether) current in systems with a global continuous symmetry. We explain how this fact leads to the existence of linear relations between Noether currents of distinct global symmetries that coincide on the local level, thus generalizing the well-known relationship $\\vec L=\\vec r\\times\\vec p$ between momentum $\\vec p$ and angular momentum $\\vec L$. As a byproduct, we find a natural interpretation for the discrepancy between the canonical and metric energy-momentum tensors in theories o","authors_text":"Tomas Brauner","cross_cats":["hep-ph","physics.class-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-10-27T09:59:09Z","title":"Noether currents of locally equivalent symmetries"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1910.12224","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:0c684571bcd72a158d531619a99552b572076650d3e1f05baafba9cbd96ece58","target":"record","created_at":"2026-07-05T00:38:46Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"ab443322a9481327b4cde12267df558d2598e2802ef79d56f0305a3076417bc7","cross_cats_sorted":["hep-ph","physics.class-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-10-27T09:59:09Z","title_canon_sha256":"d03f12eacf366cbf2b8863f4dafd759f21ddc7d20518371b0f4bb0fba8eb687a"},"schema_version":"1.0","source":{"id":"1910.12224","kind":"arxiv","version":1}},"canonical_sha256":"1226c8d3b324adf8c858acc3a89d6d2144e4beec84a9dde44c7903bb5d2e09fb","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1226c8d3b324adf8c858acc3a89d6d2144e4beec84a9dde44c7903bb5d2e09fb","first_computed_at":"2026-07-05T00:38:46.656258Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T00:38:46.656258Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"DtTLzUnmT0FhpYb0R56iirt9I9i+Kq9HZB1C/sU2uxGpDOoc48EqFOW9EQOS7FwiJaQmII2Qz9r0g1J2chiZCQ==","signature_status":"signed_v1","signed_at":"2026-07-05T00:38:46.656763Z","signed_message":"canonical_sha256_bytes"},"source_id":"1910.12224","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0c684571bcd72a158d531619a99552b572076650d3e1f05baafba9cbd96ece58","sha256:7746570fc914d6d0ccbaf638d751a9f09c11ad3d685fd925ba15bf13ebb8c3cd"],"state_sha256":"e21e82260091f0fdbbebde33bccaa8b602a01fe89671254715e0b2d7ad71f4db"}