{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:J3DHYYDP6WVSVDLJCIKRLVMDEN","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":"43038d0def74a588540071eaf81bcc677f7e60d3d2f7718ca96bac86fa00668a","cross_cats_sorted":["cond-mat.stat-mech","gr-qc","math-ph","math.MP","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2025-12-18T21:35:55Z","title_canon_sha256":"7e2f55432a53e23c71f18b16cbcebb8c3f4a4c0df59b1e2b631140064d6960de"},"schema_version":"1.0","source":{"id":"2512.17089","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2512.17089","created_at":"2026-05-25T02:02:11Z"},{"alias_kind":"arxiv_version","alias_value":"2512.17089v3","created_at":"2026-05-25T02:02:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2512.17089","created_at":"2026-05-25T02:02:11Z"},{"alias_kind":"pith_short_12","alias_value":"J3DHYYDP6WVS","created_at":"2026-05-25T02:02:11Z"},{"alias_kind":"pith_short_16","alias_value":"J3DHYYDP6WVSVDLJ","created_at":"2026-05-25T02:02:11Z"},{"alias_kind":"pith_short_8","alias_value":"J3DHYYDP","created_at":"2026-05-25T02:02:11Z"}],"graph_snapshots":[{"event_id":"sha256:b0a309307c871583faf729874942fb8f6265bf1fae17c8be82522fd90b42da24","target":"graph","created_at":"2026-05-25T02:02:11Z","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/2512.17089/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present explicit top-down calculations of Open EFTs for gauged degrees of freedom with a focus on the effects of gauge fixing. Starting from the in-in contour with two copies of the action, we integrate out the charged matter in various $U(1)$ gauge theories to obtain the Feynman-Vernon influence functional for the photon, or, in the case of symmetry breaking, for the photon and St\\\"uckelberg fields. The influence functional is defined through a quantum path integral, which -- as is always the case when quantizing gauge degrees of freedom -- contains redundancies that must be eliminated via","authors_text":"Andrew J. Tolley, Greg Kaplanek, Maria Mylova","cross_cats":["cond-mat.stat-mech","gr-qc","math-ph","math.MP","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2025-12-18T21:35:55Z","title":"Gauging Open EFTs from the top down"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2512.17089","kind":"arxiv","version":3},"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:e4729046dffffd750bffda6073b7d8690f596547ba4271cb73e69a149a00169b","target":"record","created_at":"2026-05-25T02:02:11Z","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":"43038d0def74a588540071eaf81bcc677f7e60d3d2f7718ca96bac86fa00668a","cross_cats_sorted":["cond-mat.stat-mech","gr-qc","math-ph","math.MP","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2025-12-18T21:35:55Z","title_canon_sha256":"7e2f55432a53e23c71f18b16cbcebb8c3f4a4c0df59b1e2b631140064d6960de"},"schema_version":"1.0","source":{"id":"2512.17089","kind":"arxiv","version":3}},"canonical_sha256":"4ec67c606ff5ab2a8d69121515d5832346417b1539c4022140e6eeb4e0c204de","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4ec67c606ff5ab2a8d69121515d5832346417b1539c4022140e6eeb4e0c204de","first_computed_at":"2026-05-25T02:02:11.618617Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-25T02:02:11.618617Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"FE4C3Nb8KOkWmytYoJOspREz0+cLNRcFj5LYYTEJov4YtQgpbrki0uS5DusaG7NPbCudMyzWeUQuOqdK+aHpBQ==","signature_status":"signed_v1","signed_at":"2026-05-25T02:02:11.619267Z","signed_message":"canonical_sha256_bytes"},"source_id":"2512.17089","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e4729046dffffd750bffda6073b7d8690f596547ba4271cb73e69a149a00169b","sha256:b0a309307c871583faf729874942fb8f6265bf1fae17c8be82522fd90b42da24"],"state_sha256":"c638312c2cf592823abf6e45f87100cfb0d187fc853cd4b7316bf098f81bf63f"}