{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:B6ZXDZATI2HNFPFLRGCQPWH2P7","short_pith_number":"pith:B6ZXDZAT","schema_version":"1.0","canonical_sha256":"0fb371e413468ed2bcab898507d8fa7fcac4a813e896cc2d4c4a057a0b6b510f","source":{"kind":"arxiv","id":"2101.02210","version":2},"attestation_state":"computed","paper":{"title":"Higher-form and (non-)St\\\"uckelberg symmetries in non-equilibrium systems","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.other","gr-qc","nucl-th"],"primary_cat":"hep-th","authors_text":"Michael J. Landry","submitted_at":"2021-01-06T19:00:00Z","abstract_excerpt":"We investigate the role of higher-form symmetries in non-equilibrium systems from the perspective of effective actions defined on the Schwinger-Keldysh contour. To aid our investigation, we extend the coset construction to account for $p$-form symmetries at zero and finite temperature. Additionally we investigate how, out of equilibrium, symmetries of the action need not lead to meaningful conserved currents at the level of the equations of motion. For reasons that will become apparent, we term symmetries with conserved currents St\\\"uckelberg symmetries and those without meaningful conserved c"},"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":"2101.02210","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2021-01-06T19:00:00Z","cross_cats_sorted":["cond-mat.other","gr-qc","nucl-th"],"title_canon_sha256":"d4cd3093d4b3076b2d0e74012979d5a614a798848e536baf2059cd3a03edaa3b","abstract_canon_sha256":"8921ee37c68259fa449adaa35f33cb3f09638a4c819c71c429980b5c4ede47d7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:04:37.616825Z","signature_b64":"YsVnuxBbV5Qv+khCAgKLA7rahg79qwbKBgJMdhLK3oDccD9865iJE7XpU7ErjUceC8+/buc8QrdVZEBpAfb0AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0fb371e413468ed2bcab898507d8fa7fcac4a813e896cc2d4c4a057a0b6b510f","last_reissued_at":"2026-07-05T04:04:37.616364Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:04:37.616364Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higher-form and (non-)St\\\"uckelberg symmetries in non-equilibrium systems","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.other","gr-qc","nucl-th"],"primary_cat":"hep-th","authors_text":"Michael J. Landry","submitted_at":"2021-01-06T19:00:00Z","abstract_excerpt":"We investigate the role of higher-form symmetries in non-equilibrium systems from the perspective of effective actions defined on the Schwinger-Keldysh contour. To aid our investigation, we extend the coset construction to account for $p$-form symmetries at zero and finite temperature. Additionally we investigate how, out of equilibrium, symmetries of the action need not lead to meaningful conserved currents at the level of the equations of motion. For reasons that will become apparent, we term symmetries with conserved currents St\\\"uckelberg symmetries and those without meaningful conserved c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2101.02210","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/2101.02210/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":"2101.02210","created_at":"2026-07-05T04:04:37.616421+00:00"},{"alias_kind":"arxiv_version","alias_value":"2101.02210v2","created_at":"2026-07-05T04:04:37.616421+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2101.02210","created_at":"2026-07-05T04:04:37.616421+00:00"},{"alias_kind":"pith_short_12","alias_value":"B6ZXDZATI2HN","created_at":"2026-07-05T04:04:37.616421+00:00"},{"alias_kind":"pith_short_16","alias_value":"B6ZXDZATI2HNFPFL","created_at":"2026-07-05T04:04:37.616421+00:00"},{"alias_kind":"pith_short_8","alias_value":"B6ZXDZAT","created_at":"2026-07-05T04:04:37.616421+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.21136","citing_title":"Gravitational EFT for dissipative open systems","ref_index":16,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/B6ZXDZATI2HNFPFLRGCQPWH2P7","json":"https://pith.science/pith/B6ZXDZATI2HNFPFLRGCQPWH2P7.json","graph_json":"https://pith.science/api/pith-number/B6ZXDZATI2HNFPFLRGCQPWH2P7/graph.json","events_json":"https://pith.science/api/pith-number/B6ZXDZATI2HNFPFLRGCQPWH2P7/events.json","paper":"https://pith.science/paper/B6ZXDZAT"},"agent_actions":{"view_html":"https://pith.science/pith/B6ZXDZATI2HNFPFLRGCQPWH2P7","download_json":"https://pith.science/pith/B6ZXDZATI2HNFPFLRGCQPWH2P7.json","view_paper":"https://pith.science/paper/B6ZXDZAT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2101.02210&json=true","fetch_graph":"https://pith.science/api/pith-number/B6ZXDZATI2HNFPFLRGCQPWH2P7/graph.json","fetch_events":"https://pith.science/api/pith-number/B6ZXDZATI2HNFPFLRGCQPWH2P7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/B6ZXDZATI2HNFPFLRGCQPWH2P7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/B6ZXDZATI2HNFPFLRGCQPWH2P7/action/storage_attestation","attest_author":"https://pith.science/pith/B6ZXDZATI2HNFPFLRGCQPWH2P7/action/author_attestation","sign_citation":"https://pith.science/pith/B6ZXDZATI2HNFPFLRGCQPWH2P7/action/citation_signature","submit_replication":"https://pith.science/pith/B6ZXDZATI2HNFPFLRGCQPWH2P7/action/replication_record"}},"created_at":"2026-07-05T04:04:37.616421+00:00","updated_at":"2026-07-05T04:04:37.616421+00:00"}