{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:JG5IBWRRBEY633WZO6ZSTX3GRE","short_pith_number":"pith:JG5IBWRR","canonical_record":{"source":{"id":"1805.01700","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-05-04T10:32:48Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"c89b5e2c9800c774882f84b5a9dd26b98df9d6d53017e599584d95d6163ac919","abstract_canon_sha256":"437b0d78300ae84f8e92f455fefe0317269e98413fb763b3962b7352ccb5717c"},"schema_version":"1.0"},"canonical_sha256":"49ba80da310931edeed977b329df6689396a04128360d87f0d1a7b338695a0a1","source":{"kind":"arxiv","id":"1805.01700","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1805.01700","created_at":"2026-05-18T00:09:59Z"},{"alias_kind":"arxiv_version","alias_value":"1805.01700v2","created_at":"2026-05-18T00:09:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.01700","created_at":"2026-05-18T00:09:59Z"},{"alias_kind":"pith_short_12","alias_value":"JG5IBWRRBEY6","created_at":"2026-05-18T12:32:31Z"},{"alias_kind":"pith_short_16","alias_value":"JG5IBWRRBEY633WZ","created_at":"2026-05-18T12:32:31Z"},{"alias_kind":"pith_short_8","alias_value":"JG5IBWRR","created_at":"2026-05-18T12:32:31Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:JG5IBWRRBEY633WZO6ZSTX3GRE","target":"record","payload":{"canonical_record":{"source":{"id":"1805.01700","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-05-04T10:32:48Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"c89b5e2c9800c774882f84b5a9dd26b98df9d6d53017e599584d95d6163ac919","abstract_canon_sha256":"437b0d78300ae84f8e92f455fefe0317269e98413fb763b3962b7352ccb5717c"},"schema_version":"1.0"},"canonical_sha256":"49ba80da310931edeed977b329df6689396a04128360d87f0d1a7b338695a0a1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:09:59.460451Z","signature_b64":"V/+EBpwWbBcPvyi5ACYHm8vyy1NrSOyoJIFT534XEBXfV76+L4uHDKXLnYZ067+Cg4ZU/Ku9/Hzqqa1+uBCtCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"49ba80da310931edeed977b329df6689396a04128360d87f0d1a7b338695a0a1","last_reissued_at":"2026-05-18T00:09:59.459628Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:09:59.459628Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1805.01700","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":"2026-05-18T00:09:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tTxv8JA0+1P9vynJJ27TpIGGMEgn/Q2kin+mhJHCxsU+KJlSZqvA3TXnrAoTzQ6YqpXuA0GMXDRqXB6YlhS9CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T07:42:38.521707Z"},"content_sha256":"548cc5d3c22809404fb4cb6759211ae1493aa691243ea9f1846d4c85e5ad09bb","schema_version":"1.0","event_id":"sha256:548cc5d3c22809404fb4cb6759211ae1493aa691243ea9f1846d4c85e5ad09bb"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:JG5IBWRRBEY633WZO6ZSTX3GRE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Gauged Yukawa model in curved spacetime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"David J. Toms","submitted_at":"2018-05-04T10:32:48Z","abstract_excerpt":"The Yukawa model in curved spacetime is considered. We consider a complex scalar field coupled to a $U(1)$ gauge field and also interacting with Dirac fields with a general Yukawa coupling. The local momentum space method is used to obtain the one-loop effective action and we adopt the gauge condition independent background field method introduced by Vilkovisky and DeWitt. The pole parts of the one-loop effective action that depend on the background scalar field, that we do not assume to be constant, are found and used to calculate the counterterms and to determine the relevant renormalization"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.01700","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":"2026-05-18T00:09:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sUlAhdOz8YiCIfuj1HXpacM6B+oCINu3oCa4zn4dDy/lpyrpWK2WZRkjyH0WqOUvUSbXpAqcOsjTHVAGXjRKDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T07:42:38.522454Z"},"content_sha256":"e95ebdb42a25893ee41c039c161102acf30856b128e6b5e07de4a0ee689fe86e","schema_version":"1.0","event_id":"sha256:e95ebdb42a25893ee41c039c161102acf30856b128e6b5e07de4a0ee689fe86e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JG5IBWRRBEY633WZO6ZSTX3GRE/bundle.json","state_url":"https://pith.science/pith/JG5IBWRRBEY633WZO6ZSTX3GRE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JG5IBWRRBEY633WZO6ZSTX3GRE/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":"2026-06-10T07:42:38Z","links":{"resolver":"https://pith.science/pith/JG5IBWRRBEY633WZO6ZSTX3GRE","bundle":"https://pith.science/pith/JG5IBWRRBEY633WZO6ZSTX3GRE/bundle.json","state":"https://pith.science/pith/JG5IBWRRBEY633WZO6ZSTX3GRE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JG5IBWRRBEY633WZO6ZSTX3GRE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:JG5IBWRRBEY633WZO6ZSTX3GRE","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":"437b0d78300ae84f8e92f455fefe0317269e98413fb763b3962b7352ccb5717c","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-05-04T10:32:48Z","title_canon_sha256":"c89b5e2c9800c774882f84b5a9dd26b98df9d6d53017e599584d95d6163ac919"},"schema_version":"1.0","source":{"id":"1805.01700","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1805.01700","created_at":"2026-05-18T00:09:59Z"},{"alias_kind":"arxiv_version","alias_value":"1805.01700v2","created_at":"2026-05-18T00:09:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.01700","created_at":"2026-05-18T00:09:59Z"},{"alias_kind":"pith_short_12","alias_value":"JG5IBWRRBEY6","created_at":"2026-05-18T12:32:31Z"},{"alias_kind":"pith_short_16","alias_value":"JG5IBWRRBEY633WZ","created_at":"2026-05-18T12:32:31Z"},{"alias_kind":"pith_short_8","alias_value":"JG5IBWRR","created_at":"2026-05-18T12:32:31Z"}],"graph_snapshots":[{"event_id":"sha256:e95ebdb42a25893ee41c039c161102acf30856b128e6b5e07de4a0ee689fe86e","target":"graph","created_at":"2026-05-18T00:09:59Z","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":"The Yukawa model in curved spacetime is considered. We consider a complex scalar field coupled to a $U(1)$ gauge field and also interacting with Dirac fields with a general Yukawa coupling. The local momentum space method is used to obtain the one-loop effective action and we adopt the gauge condition independent background field method introduced by Vilkovisky and DeWitt. The pole parts of the one-loop effective action that depend on the background scalar field, that we do not assume to be constant, are found and used to calculate the counterterms and to determine the relevant renormalization","authors_text":"David J. Toms","cross_cats":["gr-qc"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-05-04T10:32:48Z","title":"Gauged Yukawa model in curved spacetime"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.01700","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":"sha256:548cc5d3c22809404fb4cb6759211ae1493aa691243ea9f1846d4c85e5ad09bb","target":"record","created_at":"2026-05-18T00:09:59Z","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":"437b0d78300ae84f8e92f455fefe0317269e98413fb763b3962b7352ccb5717c","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-05-04T10:32:48Z","title_canon_sha256":"c89b5e2c9800c774882f84b5a9dd26b98df9d6d53017e599584d95d6163ac919"},"schema_version":"1.0","source":{"id":"1805.01700","kind":"arxiv","version":2}},"canonical_sha256":"49ba80da310931edeed977b329df6689396a04128360d87f0d1a7b338695a0a1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"49ba80da310931edeed977b329df6689396a04128360d87f0d1a7b338695a0a1","first_computed_at":"2026-05-18T00:09:59.459628Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:09:59.459628Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"V/+EBpwWbBcPvyi5ACYHm8vyy1NrSOyoJIFT534XEBXfV76+L4uHDKXLnYZ067+Cg4ZU/Ku9/Hzqqa1+uBCtCg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:09:59.460451Z","signed_message":"canonical_sha256_bytes"},"source_id":"1805.01700","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:548cc5d3c22809404fb4cb6759211ae1493aa691243ea9f1846d4c85e5ad09bb","sha256:e95ebdb42a25893ee41c039c161102acf30856b128e6b5e07de4a0ee689fe86e"],"state_sha256":"f92b19f9c5bd8e4417aaeefb54a1442385fab00271bab33e5ea83ad1946a794a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lOBmnpRqJdQEGn5l0rJNfPbEE9sbqCiqxEeV3Mc3tuwzF2EJzcvNUnKBHlNZSFxUzi9k9WzQ37jucs4mDOWsCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-10T07:42:38.526432Z","bundle_sha256":"d5f4924e622a35759631a65e942ea7c29c472e4bb19edb8323105160b766f496"}}