{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:KOITDP7P4RN2GBIP2K5Y2JLPDN","short_pith_number":"pith:KOITDP7P","canonical_record":{"source":{"id":"2605.14245","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2026-05-14T01:22:19Z","cross_cats_sorted":[],"title_canon_sha256":"a9b11c526821ca5b6479c59c774ad6df0c72b6acf72b0b25f1513d7f4926ec0f","abstract_canon_sha256":"62423e415c27c9204b7184c139d5fe734c5363f9a5c2f48faf3ae79394358791"},"schema_version":"1.0"},"canonical_sha256":"539131bfefe45ba3050fd2bb8d256f1b7da6e5430145d637fd56fa0b61771df1","source":{"kind":"arxiv","id":"2605.14245","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.14245","created_at":"2026-05-17T23:39:10Z"},{"alias_kind":"arxiv_version","alias_value":"2605.14245v1","created_at":"2026-05-17T23:39:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.14245","created_at":"2026-05-17T23:39:10Z"},{"alias_kind":"pith_short_12","alias_value":"KOITDP7P4RN2","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_16","alias_value":"KOITDP7P4RN2GBIP","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_8","alias_value":"KOITDP7P","created_at":"2026-05-18T12:33:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:KOITDP7P4RN2GBIP2K5Y2JLPDN","target":"record","payload":{"canonical_record":{"source":{"id":"2605.14245","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2026-05-14T01:22:19Z","cross_cats_sorted":[],"title_canon_sha256":"a9b11c526821ca5b6479c59c774ad6df0c72b6acf72b0b25f1513d7f4926ec0f","abstract_canon_sha256":"62423e415c27c9204b7184c139d5fe734c5363f9a5c2f48faf3ae79394358791"},"schema_version":"1.0"},"canonical_sha256":"539131bfefe45ba3050fd2bb8d256f1b7da6e5430145d637fd56fa0b61771df1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:39:10.618899Z","signature_b64":"EvK9iqBA9Qwt0bdkNJpt0sgXVQ67RsG4QVcMqvvCpaP0lGnePJYuc2n23oWGXO2hegkVs5ZLQ0cPSoXrdrDGBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"539131bfefe45ba3050fd2bb8d256f1b7da6e5430145d637fd56fa0b61771df1","last_reissued_at":"2026-05-17T23:39:10.618403Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:39:10.618403Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2605.14245","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:39:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CSxeR4jVrNKTWYnIvIlm5Gd1agKgc+Nrj6tcY8uSplnZ6vJnpevYXKQI4LlOs+P6PmCh4TM6CQkO2ZgKLnHXAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T09:03:56.757672Z"},"content_sha256":"cd452cbaf403d3176e856c78eb44994febca1d393544accc3739df5c1b891d80","schema_version":"1.0","event_id":"sha256:cd452cbaf403d3176e856c78eb44994febca1d393544accc3739df5c1b891d80"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:KOITDP7P4RN2GBIP2K5Y2JLPDN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Constraints on anomalous Higgs boson couplings to vector bosons and fermions using the $\\gamma\\gamma$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"Updated constraints from the full Run 2 dataset show no evidence for anomalous Higgs couplings in gluon fusion, vector boson fusion, and associated production modes decaying to two photons.","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2026-05-14T01:22:19Z","abstract_excerpt":"Possible anomalous couplings of the Higgs boson to vector bosons and fermions are studied using Higgs boson candidates decaying to a pair of photons. The study is based on proton-proton collision data at $\\sqrt{s}$ = 13 TeV collected by the CMS experiment, corresponding to an integrated luminosity of 138 fb$^{-1}$. Events with Higgs boson candidates produced via gluon fusion, electroweak vector boson fusion and in association with a vector boson, are categorized using matrix element techniques and multivariate discriminants. The $CP$ properties of the Higgs boson couplings to gluons through lo"},"claims":{"count":3,"items":[{"kind":"strongest_claim","text":"The results are interpreted in terms of the fractional contributions of anomalous Higgs boson couplings to the total production cross section of each process and are found to be consistent with the standard model expectations.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"The matrix element techniques and multivariate discriminants correctly categorize events and separate signal from background without significant bias from unmodeled effects.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"Updated constraints from the full Run 2 dataset show no evidence for anomalous Higgs couplings in gluon fusion, vector boson fusion, and associated production modes decaying to two photons.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"}],"snapshot_sha256":"3083d2ff68222d2963164e98419c7dfe7d7d238c30ba55456a93223bd0d753d1"},"source":{"id":"2605.14245","kind":"arxiv","version":1},"verdict":{"id":"4d1a2226-e18b-429a-9055-4969bc149936","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-15T02:16:49.728489Z","strongest_claim":"The results are interpreted in terms of the fractional contributions of anomalous Higgs boson couplings to the total production cross section of each process and are found to be consistent with the standard model expectations.","one_line_summary":"Updated constraints from the full Run 2 dataset show no evidence for anomalous Higgs couplings in gluon fusion, vector boson fusion, and associated production modes decaying to two photons.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"The matrix element techniques and multivariate discriminants correctly categorize events and separate signal from background without significant bias from unmodeled effects.","pith_extraction_headline":""},"references":{"count":93,"sample":[{"doi":"10.1016/j.physletb.2012.08.020","year":2012,"title":"Observation of a new particle in the search for the standard model higgs boson with the atlas detector at the lhc.Physics Letters B2012;716(1):1–29","work_id":"ecf87d7b-ffee-4edd-a7cd-56371de672ff","ref_index":1,"cited_arxiv_id":"1207.7214","is_internal_anchor":true},{"doi":"10.1016/j.physletb.2012.08.021","year":2012,"title":"Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC","work_id":"02ab5f35-5521-45e2-bb51-6c2b69b1c615","ref_index":2,"cited_arxiv_id":"1207.7235","is_internal_anchor":true},{"doi":"10.1007/jhep06(2013)081","year":2013,"title":"Observation of a new boson with mass near 125 GeV in pp collisions at sqrt(s) = 7 and 8 TeV","work_id":"bf7a82ba-af89-47f3-9c46-6608f5df8a87","ref_index":3,"cited_arxiv_id":"1303.4571","is_internal_anchor":true},{"doi":"10.1016/0029-5582(61)90469-2","year":1961,"title":"Partial-symmetries of weak interactions","work_id":"816ced38-9e55-43ef-a88e-beef42c8adaa","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"10.1103/physrevlett.13.321","year":1964,"title":"Phys.Rev.Lett.13 (1964) 321","work_id":"7c623f60-c747-4a7b-b3f5-9f94f32caed4","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":93,"snapshot_sha256":"d25e9c383932ac85ee38f115d6bc8db8b1fb41fad551563a2eafe47e3542cef3","internal_anchors":51},"formal_canon":{"evidence_count":2,"snapshot_sha256":"32a4e40a3a8572c8a2e88a8a64be23d6024ab0aae3d4efa7a295ec6090ee3f6b"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":"4d1a2226-e18b-429a-9055-4969bc149936"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:39:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Gcy/m0iej2p0lHVabQNFJZ/57DOnSnNIL0vPoZcbBbfRhxURY74Cq/M9AN/ZElb32tdf9AgPbfmkn1j7gU1jCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T09:03:56.758308Z"},"content_sha256":"019ff9560407a06662c4a29dea4238da1d2b47a15b789d58ee8f236ccccc5796","schema_version":"1.0","event_id":"sha256:019ff9560407a06662c4a29dea4238da1d2b47a15b789d58ee8f236ccccc5796"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:KOITDP7P4RN2GBIP2K5Y2JLPDN","target":"integrity","payload":{"note":"Identifier '10.17182/hepdata.169546' is syntactically valid but the DOI registry (doi.org) returned 404, and Crossref / OpenAlex / internal corpus also have no record. The cited work could not be located through any authoritative source.","snippet":"HEPData record for this analysis, 2026.doi:10.17182/hepdata.169546","arxiv_id":"2605.14245","detector":"doi_compliance","evidence":{"doi":"10.17182/hepdata.169546","arxiv_id":null,"ref_index":37,"raw_excerpt":"HEPData record for this analysis, 2026.doi:10.17182/hepdata.169546","verdict_class":"cross_source","checked_sources":["crossref_by_doi","openalex_by_doi","doi_org_head"]},"severity":"critical","ref_index":37,"audited_at":"2026-05-19T05:43:03.597974Z","event_type":"pith.integrity.v1","detected_doi":"10.17182/hepdata.169546","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"unresolvable_identifier","evidence_hash":"1acf963d79a2738f999e545b9f2009ba0ca4569b50fdd22a84c355b0ceaf9e49","paper_version":1,"verdict_class":"cross_source","resolved_title":null,"detector_version":"1.0.0","detected_arxiv_id":null,"integrity_event_id":43,"payload_sha256":"1f0c69355b20458f23ee58d1d605981b12bb41f07abccf11ce4c69088df8e0c4","signature_b64":"zGTojJibfWII3niTWjZ5uyMGAmLsh/EgdXGzcV8dD8ZRqrlRPjUU7JifocAIfvqKzEG9YYC8Tl1HMkpoTzzsCw==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-19T05:46:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3xE9bAbW+3kqiF5LlfrZ6nQjCJDbzHgrI6Q4snMOqblFQOEpVkmziiX7M+1pNF13QfnvZJ75+zYYs/jn3SqgAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T09:03:56.759177Z"},"content_sha256":"0ce90f5d14669e1e7dc94b882d31c5c7ffb77de4747032b0919cdb29989fba2e","schema_version":"1.0","event_id":"sha256:0ce90f5d14669e1e7dc94b882d31c5c7ffb77de4747032b0919cdb29989fba2e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KOITDP7P4RN2GBIP2K5Y2JLPDN/bundle.json","state_url":"https://pith.science/pith/KOITDP7P4RN2GBIP2K5Y2JLPDN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KOITDP7P4RN2GBIP2K5Y2JLPDN/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":"2026-05-21T09:03:56Z","links":{"resolver":"https://pith.science/pith/KOITDP7P4RN2GBIP2K5Y2JLPDN","bundle":"https://pith.science/pith/KOITDP7P4RN2GBIP2K5Y2JLPDN/bundle.json","state":"https://pith.science/pith/KOITDP7P4RN2GBIP2K5Y2JLPDN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KOITDP7P4RN2GBIP2K5Y2JLPDN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:KOITDP7P4RN2GBIP2K5Y2JLPDN","merge_version":"pith-open-graph-merge-v1","event_count":3,"valid_event_count":3,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"62423e415c27c9204b7184c139d5fe734c5363f9a5c2f48faf3ae79394358791","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2026-05-14T01:22:19Z","title_canon_sha256":"a9b11c526821ca5b6479c59c774ad6df0c72b6acf72b0b25f1513d7f4926ec0f"},"schema_version":"1.0","source":{"id":"2605.14245","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.14245","created_at":"2026-05-17T23:39:10Z"},{"alias_kind":"arxiv_version","alias_value":"2605.14245v1","created_at":"2026-05-17T23:39:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.14245","created_at":"2026-05-17T23:39:10Z"},{"alias_kind":"pith_short_12","alias_value":"KOITDP7P4RN2","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_16","alias_value":"KOITDP7P4RN2GBIP","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_8","alias_value":"KOITDP7P","created_at":"2026-05-18T12:33:37Z"}],"graph_snapshots":[{"event_id":"sha256:019ff9560407a06662c4a29dea4238da1d2b47a15b789d58ee8f236ccccc5796","target":"graph","created_at":"2026-05-17T23:39:10Z","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":3,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","text":"The results are interpreted in terms of the fractional contributions of anomalous Higgs boson couplings to the total production cross section of each process and are found to be consistent with the standard model expectations."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"The matrix element techniques and multivariate discriminants correctly categorize events and separate signal from background without significant bias from unmodeled effects."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"Updated constraints from the full Run 2 dataset show no evidence for anomalous Higgs couplings in gluon fusion, vector boson fusion, and associated production modes decaying to two photons."}],"snapshot_sha256":"3083d2ff68222d2963164e98419c7dfe7d7d238c30ba55456a93223bd0d753d1"},"formal_canon":{"evidence_count":2,"snapshot_sha256":"32a4e40a3a8572c8a2e88a8a64be23d6024ab0aae3d4efa7a295ec6090ee3f6b"},"paper":{"abstract_excerpt":"Possible anomalous couplings of the Higgs boson to vector bosons and fermions are studied using Higgs boson candidates decaying to a pair of photons. The study is based on proton-proton collision data at $\\sqrt{s}$ = 13 TeV collected by the CMS experiment, corresponding to an integrated luminosity of 138 fb$^{-1}$. Events with Higgs boson candidates produced via gluon fusion, electroweak vector boson fusion and in association with a vector boson, are categorized using matrix element techniques and multivariate discriminants. The $CP$ properties of the Higgs boson couplings to gluons through lo","authors_text":"CMS Collaboration","cross_cats":[],"headline":"Updated constraints from the full Run 2 dataset show no evidence for anomalous Higgs couplings in gluon fusion, vector boson fusion, and associated production modes decaying to two photons.","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2026-05-14T01:22:19Z","title":"Constraints on anomalous Higgs boson couplings to vector bosons and fermions using the $\\gamma\\gamma$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV"},"references":{"count":93,"internal_anchors":51,"resolved_work":93,"sample":[{"cited_arxiv_id":"1207.7214","doi":"10.1016/j.physletb.2012.08.020","is_internal_anchor":true,"ref_index":1,"title":"Observation of a new particle in the search for the standard model higgs boson with the atlas detector at the lhc.Physics Letters B2012;716(1):1–29","work_id":"ecf87d7b-ffee-4edd-a7cd-56371de672ff","year":2012},{"cited_arxiv_id":"1207.7235","doi":"10.1016/j.physletb.2012.08.021","is_internal_anchor":true,"ref_index":2,"title":"Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC","work_id":"02ab5f35-5521-45e2-bb51-6c2b69b1c615","year":2012},{"cited_arxiv_id":"1303.4571","doi":"10.1007/jhep06(2013)081","is_internal_anchor":true,"ref_index":3,"title":"Observation of a new boson with mass near 125 GeV in pp collisions at sqrt(s) = 7 and 8 TeV","work_id":"bf7a82ba-af89-47f3-9c46-6608f5df8a87","year":2013},{"cited_arxiv_id":"","doi":"10.1016/0029-5582(61)90469-2","is_internal_anchor":false,"ref_index":4,"title":"Partial-symmetries of weak interactions","work_id":"816ced38-9e55-43ef-a88e-beef42c8adaa","year":1961},{"cited_arxiv_id":"","doi":"10.1103/physrevlett.13.321","is_internal_anchor":false,"ref_index":5,"title":"Phys.Rev.Lett.13 (1964) 321","work_id":"7c623f60-c747-4a7b-b3f5-9f94f32caed4","year":1964}],"snapshot_sha256":"d25e9c383932ac85ee38f115d6bc8db8b1fb41fad551563a2eafe47e3542cef3"},"source":{"id":"2605.14245","kind":"arxiv","version":1},"verdict":{"created_at":"2026-05-15T02:16:49.728489Z","id":"4d1a2226-e18b-429a-9055-4969bc149936","model_set":{"reader":"grok-4.3"},"one_line_summary":"Updated constraints from the full Run 2 dataset show no evidence for anomalous Higgs couplings in gluon fusion, vector boson fusion, and associated production modes decaying to two photons.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"","strongest_claim":"The results are interpreted in terms of the fractional contributions of anomalous Higgs boson couplings to the total production cross section of each process and are found to be consistent with the standard model expectations.","weakest_assumption":"The matrix element techniques and multivariate discriminants correctly categorize events and separate signal from background without significant bias from unmodeled effects."}},"verdict_id":"4d1a2226-e18b-429a-9055-4969bc149936"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:cd452cbaf403d3176e856c78eb44994febca1d393544accc3739df5c1b891d80","target":"record","created_at":"2026-05-17T23:39:10Z","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":"62423e415c27c9204b7184c139d5fe734c5363f9a5c2f48faf3ae79394358791","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2026-05-14T01:22:19Z","title_canon_sha256":"a9b11c526821ca5b6479c59c774ad6df0c72b6acf72b0b25f1513d7f4926ec0f"},"schema_version":"1.0","source":{"id":"2605.14245","kind":"arxiv","version":1}},"canonical_sha256":"539131bfefe45ba3050fd2bb8d256f1b7da6e5430145d637fd56fa0b61771df1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"539131bfefe45ba3050fd2bb8d256f1b7da6e5430145d637fd56fa0b61771df1","first_computed_at":"2026-05-17T23:39:10.618403Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:39:10.618403Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"EvK9iqBA9Qwt0bdkNJpt0sgXVQ67RsG4QVcMqvvCpaP0lGnePJYuc2n23oWGXO2hegkVs5ZLQ0cPSoXrdrDGBg==","signature_status":"signed_v1","signed_at":"2026-05-17T23:39:10.618899Z","signed_message":"canonical_sha256_bytes"},"source_id":"2605.14245","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cd452cbaf403d3176e856c78eb44994febca1d393544accc3739df5c1b891d80","sha256:019ff9560407a06662c4a29dea4238da1d2b47a15b789d58ee8f236ccccc5796","sha256:0ce90f5d14669e1e7dc94b882d31c5c7ffb77de4747032b0919cdb29989fba2e"],"state_sha256":"5c35cd242f0c7f62c02b71496c2e007e67c26d90b0dad9d46e344a7932493430"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+DMGY1kf0JgheG+f7raWa4lCzo0MgUq9PDtsgl36nhr5XjBCNkv7CvrYjw3cS7zZ78xIV+e68gupCNh0nXZRCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-21T09:03:56.761665Z","bundle_sha256":"caf8471cbe827501d9fa5f7baca5957d44cb273071726fc2e9c7ee02706dacda"}}