{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:FPTE2HHZA4VU5PSIYILZ4P6EVQ","short_pith_number":"pith:FPTE2HHZ","canonical_record":{"source":{"id":"1812.06093","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2018-12-14T19:00:00Z","cross_cats_sorted":[],"title_canon_sha256":"3dd523c732611fe79f511bf5f6cf0f78259c6c95766b5913efbd87834dbb3b9a","abstract_canon_sha256":"2bef5acbd9eb9c5d8236d122c39693595f3fe2d0511f95137ef53d921a4a5319"},"schema_version":"1.0"},"canonical_sha256":"2be64d1cf9072b4ebe48c2179e3fc4ac17799546f7756bda354555fca2e55ec3","source":{"kind":"arxiv","id":"1812.06093","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1812.06093","created_at":"2026-05-17T23:42:25Z"},{"alias_kind":"arxiv_version","alias_value":"1812.06093v2","created_at":"2026-05-17T23:42:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.06093","created_at":"2026-05-17T23:42:25Z"},{"alias_kind":"pith_short_12","alias_value":"FPTE2HHZA4VU","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_16","alias_value":"FPTE2HHZA4VU5PSI","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_8","alias_value":"FPTE2HHZ","created_at":"2026-05-18T12:32:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:FPTE2HHZA4VU5PSIYILZ4P6EVQ","target":"record","payload":{"canonical_record":{"source":{"id":"1812.06093","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2018-12-14T19:00:00Z","cross_cats_sorted":[],"title_canon_sha256":"3dd523c732611fe79f511bf5f6cf0f78259c6c95766b5913efbd87834dbb3b9a","abstract_canon_sha256":"2bef5acbd9eb9c5d8236d122c39693595f3fe2d0511f95137ef53d921a4a5319"},"schema_version":"1.0"},"canonical_sha256":"2be64d1cf9072b4ebe48c2179e3fc4ac17799546f7756bda354555fca2e55ec3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:42:25.697554Z","signature_b64":"TeEAJyfRm81C1MIqiGFTBAFmoCGR299w5xqWKTLTLO8yPmEiwRj0SngyKDSVe/37mASFp/bnF37XxDJAcWXbCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2be64d1cf9072b4ebe48c2179e3fc4ac17799546f7756bda354555fca2e55ec3","last_reissued_at":"2026-05-17T23:42:25.696895Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:42:25.696895Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1812.06093","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:42:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Tk0sBiKlum2qOKcB7NYim224u+X/XPuiBGwZ/oEirCbHmx2IwLXSjUkHbV/j8UoqaPYagPjO15sQtwLqGoUlAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T09:25:40.869421Z"},"content_sha256":"cf321516e3c6f7cd9b947c3b08f64304353fc4f539ce89dc211bae8364af762f","schema_version":"1.0","event_id":"sha256:cf321516e3c6f7cd9b947c3b08f64304353fc4f539ce89dc211bae8364af762f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:FPTE2HHZA4VU5PSIYILZ4P6EVQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Holographic Schwinger-Keldysh effective field theories","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Jan de Boer, Michal P. Heller, Natalia Pinzani-Fokeeva","submitted_at":"2018-12-14T19:00:00Z","abstract_excerpt":"We construct a holographic dual of the Schwinger-Keldysh effective action for the dissipative low-energy dynamics of relativistic charged matter at strong coupling in a fixed thermal background. To do so, we use a mixed signature bulk spacetime whereby an eternal asymptotically anti-de Sitter black hole is glued to its Euclidean counterpart along an initial time slice in a way to match the desired double-time contour of the dual field theory. Our results are consistent with existing literature and can be regarded as a fully-ab initio derivation of a Schwinger-Keldysh effective action. In addit"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.06093","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":""},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:42:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"evOFiKO+zpSUq7101lSQm06wkime7gVo57ZgqeWgwjywJXhbbkfeHGsrREphGI2NV5c63MlMNX2K+MVdT8bJCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T09:25:40.869780Z"},"content_sha256":"6483b7c3e2e7ee5834f86f72123717406cf07a2213337411fd2edd34f321e276","schema_version":"1.0","event_id":"sha256:6483b7c3e2e7ee5834f86f72123717406cf07a2213337411fd2edd34f321e276"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FPTE2HHZA4VU5PSIYILZ4P6EVQ/bundle.json","state_url":"https://pith.science/pith/FPTE2HHZA4VU5PSIYILZ4P6EVQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FPTE2HHZA4VU5PSIYILZ4P6EVQ/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-28T09:25:40Z","links":{"resolver":"https://pith.science/pith/FPTE2HHZA4VU5PSIYILZ4P6EVQ","bundle":"https://pith.science/pith/FPTE2HHZA4VU5PSIYILZ4P6EVQ/bundle.json","state":"https://pith.science/pith/FPTE2HHZA4VU5PSIYILZ4P6EVQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FPTE2HHZA4VU5PSIYILZ4P6EVQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:FPTE2HHZA4VU5PSIYILZ4P6EVQ","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":"2bef5acbd9eb9c5d8236d122c39693595f3fe2d0511f95137ef53d921a4a5319","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2018-12-14T19:00:00Z","title_canon_sha256":"3dd523c732611fe79f511bf5f6cf0f78259c6c95766b5913efbd87834dbb3b9a"},"schema_version":"1.0","source":{"id":"1812.06093","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1812.06093","created_at":"2026-05-17T23:42:25Z"},{"alias_kind":"arxiv_version","alias_value":"1812.06093v2","created_at":"2026-05-17T23:42:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.06093","created_at":"2026-05-17T23:42:25Z"},{"alias_kind":"pith_short_12","alias_value":"FPTE2HHZA4VU","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_16","alias_value":"FPTE2HHZA4VU5PSI","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_8","alias_value":"FPTE2HHZ","created_at":"2026-05-18T12:32:25Z"}],"graph_snapshots":[{"event_id":"sha256:6483b7c3e2e7ee5834f86f72123717406cf07a2213337411fd2edd34f321e276","target":"graph","created_at":"2026-05-17T23:42:25Z","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"},"paper":{"abstract_excerpt":"We construct a holographic dual of the Schwinger-Keldysh effective action for the dissipative low-energy dynamics of relativistic charged matter at strong coupling in a fixed thermal background. To do so, we use a mixed signature bulk spacetime whereby an eternal asymptotically anti-de Sitter black hole is glued to its Euclidean counterpart along an initial time slice in a way to match the desired double-time contour of the dual field theory. Our results are consistent with existing literature and can be regarded as a fully-ab initio derivation of a Schwinger-Keldysh effective action. In addit","authors_text":"Jan de Boer, Michal P. Heller, Natalia Pinzani-Fokeeva","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2018-12-14T19:00:00Z","title":"Holographic Schwinger-Keldysh effective field theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.06093","kind":"arxiv","version":2},"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:cf321516e3c6f7cd9b947c3b08f64304353fc4f539ce89dc211bae8364af762f","target":"record","created_at":"2026-05-17T23:42:25Z","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":"2bef5acbd9eb9c5d8236d122c39693595f3fe2d0511f95137ef53d921a4a5319","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2018-12-14T19:00:00Z","title_canon_sha256":"3dd523c732611fe79f511bf5f6cf0f78259c6c95766b5913efbd87834dbb3b9a"},"schema_version":"1.0","source":{"id":"1812.06093","kind":"arxiv","version":2}},"canonical_sha256":"2be64d1cf9072b4ebe48c2179e3fc4ac17799546f7756bda354555fca2e55ec3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2be64d1cf9072b4ebe48c2179e3fc4ac17799546f7756bda354555fca2e55ec3","first_computed_at":"2026-05-17T23:42:25.696895Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:42:25.696895Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"TeEAJyfRm81C1MIqiGFTBAFmoCGR299w5xqWKTLTLO8yPmEiwRj0SngyKDSVe/37mASFp/bnF37XxDJAcWXbCg==","signature_status":"signed_v1","signed_at":"2026-05-17T23:42:25.697554Z","signed_message":"canonical_sha256_bytes"},"source_id":"1812.06093","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cf321516e3c6f7cd9b947c3b08f64304353fc4f539ce89dc211bae8364af762f","sha256:6483b7c3e2e7ee5834f86f72123717406cf07a2213337411fd2edd34f321e276"],"state_sha256":"249d77118e12ac2af4d60f9cae99262742885a05f1c811353851ce685f052d51"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RFcZ8wiY8vITxShb6qYz7dok+p6sw+TyCOSSgT5dttW+IyFQqTHHhVLzcDzGMVJcmUgrZwdOAG+TJmCJHl1JBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T09:25:40.871731Z","bundle_sha256":"64eb76695b0c4d5176697c5a4d526cd61ee050f35aec9dfa0c01df58a77c9faa"}}