{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:2BQJRWCPFOF6MIDCTQO34CXLFD","short_pith_number":"pith:2BQJRWCP","canonical_record":{"source":{"id":"2601.05312","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-01-08T19:00:01Z","cross_cats_sorted":[],"title_canon_sha256":"a04b4fa81878d7c2c2f283e2c2cd3114653291015065d8187cab776881a1926e","abstract_canon_sha256":"e7f28bad5b882501464e05a684d2bafd4d49e36b104ec4248a500ba33f2e7c01"},"schema_version":"1.0"},"canonical_sha256":"d06098d84f2b8be620629c1dbe0aeb28e541eaabe44d2ee2a67daafca49a6b2f","source":{"kind":"arxiv","id":"2601.05312","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2601.05312","created_at":"2026-05-18T02:45:12Z"},{"alias_kind":"arxiv_version","alias_value":"2601.05312v3","created_at":"2026-05-18T02:45:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2601.05312","created_at":"2026-05-18T02:45:12Z"},{"alias_kind":"pith_short_12","alias_value":"2BQJRWCPFOF6","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_16","alias_value":"2BQJRWCPFOF6MIDC","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_8","alias_value":"2BQJRWCP","created_at":"2026-05-18T12:33:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:2BQJRWCPFOF6MIDCTQO34CXLFD","target":"record","payload":{"canonical_record":{"source":{"id":"2601.05312","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-01-08T19:00:01Z","cross_cats_sorted":[],"title_canon_sha256":"a04b4fa81878d7c2c2f283e2c2cd3114653291015065d8187cab776881a1926e","abstract_canon_sha256":"e7f28bad5b882501464e05a684d2bafd4d49e36b104ec4248a500ba33f2e7c01"},"schema_version":"1.0"},"canonical_sha256":"d06098d84f2b8be620629c1dbe0aeb28e541eaabe44d2ee2a67daafca49a6b2f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:45:12.087470Z","signature_b64":"A9G6gwEmkMGt8fWaN/tZeIRMHZiZ0PRztwUC4HKQOF9zpbGcwhGrruUi1xzAJWOfgUU2e127uuUZyrZnh0IhBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d06098d84f2b8be620629c1dbe0aeb28e541eaabe44d2ee2a67daafca49a6b2f","last_reissued_at":"2026-05-18T02:45:12.086904Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:45:12.086904Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2601.05312","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:45:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SQ5BxJVWZWnSM2VgLT1Gt1rWzZTcshhkMhEh3iBAmc2VlgbidvvhRww52hKKJa3YJih0LEq0KfqMw40/LjTsCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T04:09:49.355057Z"},"content_sha256":"a1d0615e38fdc4f760b8d899aae329f489257545938fbf8fff4850a66c1a5f19","schema_version":"1.0","event_id":"sha256:a1d0615e38fdc4f760b8d899aae329f489257545938fbf8fff4850a66c1a5f19"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:2BQJRWCPFOF6MIDCTQO34CXLFD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Energy-Energy Correlator from the AdS Virasoro-Shapiro Amplitude","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"The world-sheet integral of the AdS Virasoro-Shapiro amplitude directly equals the energy-energy correlator in strongly coupled N=4 super Yang-Mills.","cross_cats":[],"primary_cat":"hep-th","authors_text":"Bo Wang, Congkao Wen, Lecheng Ren","submitted_at":"2026-01-08T19:00:01Z","abstract_excerpt":"We establish a precise formula relating the world-sheet integral of the AdS Virasoro-Shapiro amplitude to the energy-energy correlator (EEC) in $\\mathcal{N}=4$ super Yang-Mills theory at strong coupling. This mapping allows us to evaluate the coefficients of the AdS curvature expansion of the EEC in terms of the world-sheet integral over a unit disk. To illustrate this idea, we explicitly compute the flat-space contribution and the first curvature correction to the EEC. Our results provide a rigorous description of the stringy energy flow, demonstrating how world-sheet correlators imprint them"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"We establish a precise formula relating the world-sheet integral of the AdS Virasoro-Shapiro amplitude to the energy-energy correlator (EEC) in N=4 super Yang-Mills theory at strong coupling.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"The assumption that the world-sheet integral of the AdS Virasoro-Shapiro amplitude directly equals the EEC via the AdS/CFT correspondence in the strong-coupling limit.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"A precise mapping from the world-sheet integral of the AdS Virasoro-Shapiro amplitude to the energy-energy correlator in strongly coupled N=4 SYM, with explicit flat-space and first curvature correction terms.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"The world-sheet integral of the AdS Virasoro-Shapiro amplitude directly equals the energy-energy correlator in strongly coupled N=4 super Yang-Mills.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"12fcc985eea6e35bec2d952f5fb5cca6b32a00cbde37f8ea31ab9a0da522529b"},"source":{"id":"2601.05312","kind":"arxiv","version":3},"verdict":{"id":"183c17a0-288a-4b6a-9739-21aba6ac1b1e","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-16T15:45:44.402487Z","strongest_claim":"We establish a precise formula relating the world-sheet integral of the AdS Virasoro-Shapiro amplitude to the energy-energy correlator (EEC) in N=4 super Yang-Mills theory at strong coupling.","one_line_summary":"A precise mapping from the world-sheet integral of the AdS Virasoro-Shapiro amplitude to the energy-energy correlator in strongly coupled N=4 SYM, with explicit flat-space and first curvature correction terms.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"The assumption that the world-sheet integral of the AdS Virasoro-Shapiro amplitude directly equals the EEC via the AdS/CFT correspondence in the strong-coupling limit.","pith_extraction_headline":"The world-sheet integral of the AdS Virasoro-Shapiro amplitude directly equals the energy-energy correlator in strongly coupled N=4 super Yang-Mills."},"references":{"count":68,"sample":[{"doi":"","year":1978,"title":"C. L. Basham, L. S. Brown, S. D. Ellis, and S. T. Love, Energy Correlations in electron - Positron Annihilation: Testing QCD, Phys. Rev. Lett.41, 1585 (1978)","work_id":"339a5aee-7c2e-4090-be91-b0b72170deaa","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2018,"title":"C. L. Basham, L. S. Brown, S. D. Ellis, and S. T. Love, Energy Correlations in electron-Positron Annihilation in Quantum Chromodynamics: Asymptotically Free Per- turbation Theory, Phys. Rev. D19, 2018","work_id":"b5d39377-54d1-49e6-b8c7-a2e511968152","ref_index":2,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2020,"title":"H. Chen, I. Moult, X. Zhang, and H. X. Zhu, Rethinking jets with energy correlators: Tracks, resummation, and analytic continuation, Phys. Rev. D102, 054012 (2020), arXiv:2004.11381 [hep-ph]","work_id":"92a3b463-f7e5-4724-b677-a945c1e15119","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2023,"title":"P. T. Komiske, I. Moult, J. Thaler, and H. X. Zhu, Analyzing N-Point Energy Correlators inside Jets with CMS Open Data, Phys. Rev. Lett.130, 051901 (2023), arXiv:2201.07800 [hep-ph]","work_id":"82770c84-1678-4493-b1fe-bd77eaef85f0","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2025,"title":"Energy Correlators: A Journey From Theory to Experiment,","work_id":"e0b906f9-98ac-4435-b30b-e10dfb0c9afb","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":68,"snapshot_sha256":"a45efd67a4528e643699c0523105fbcde4e9ba7f5420bd58492c5fb1d2e54740","internal_anchors":17},"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":"183c17a0-288a-4b6a-9739-21aba6ac1b1e"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:45:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hZxYof88iQ9j6IXalK/vVHJjL1YTY1DZZ1qk79uHpgbPrTEzqDhZsRROGz0t1hNcS5CYFH1qpGLbz8zDuzTACQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T04:09:49.355599Z"},"content_sha256":"3a84d34a9a9cc1dd0b1f137405e848c753ebd04bbf06d60047c88bbb82a64b14","schema_version":"1.0","event_id":"sha256:3a84d34a9a9cc1dd0b1f137405e848c753ebd04bbf06d60047c88bbb82a64b14"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2BQJRWCPFOF6MIDCTQO34CXLFD/bundle.json","state_url":"https://pith.science/pith/2BQJRWCPFOF6MIDCTQO34CXLFD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2BQJRWCPFOF6MIDCTQO34CXLFD/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":"2026-05-28T04:09:49Z","links":{"resolver":"https://pith.science/pith/2BQJRWCPFOF6MIDCTQO34CXLFD","bundle":"https://pith.science/pith/2BQJRWCPFOF6MIDCTQO34CXLFD/bundle.json","state":"https://pith.science/pith/2BQJRWCPFOF6MIDCTQO34CXLFD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2BQJRWCPFOF6MIDCTQO34CXLFD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:2BQJRWCPFOF6MIDCTQO34CXLFD","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":"e7f28bad5b882501464e05a684d2bafd4d49e36b104ec4248a500ba33f2e7c01","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-01-08T19:00:01Z","title_canon_sha256":"a04b4fa81878d7c2c2f283e2c2cd3114653291015065d8187cab776881a1926e"},"schema_version":"1.0","source":{"id":"2601.05312","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2601.05312","created_at":"2026-05-18T02:45:12Z"},{"alias_kind":"arxiv_version","alias_value":"2601.05312v3","created_at":"2026-05-18T02:45:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2601.05312","created_at":"2026-05-18T02:45:12Z"},{"alias_kind":"pith_short_12","alias_value":"2BQJRWCPFOF6","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_16","alias_value":"2BQJRWCPFOF6MIDC","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_8","alias_value":"2BQJRWCP","created_at":"2026-05-18T12:33:37Z"}],"graph_snapshots":[{"event_id":"sha256:3a84d34a9a9cc1dd0b1f137405e848c753ebd04bbf06d60047c88bbb82a64b14","target":"graph","created_at":"2026-05-18T02:45:12Z","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":4,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","text":"We establish a precise formula relating the world-sheet integral of the AdS Virasoro-Shapiro amplitude to the energy-energy correlator (EEC) in N=4 super Yang-Mills theory at strong coupling."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"The assumption that the world-sheet integral of the AdS Virasoro-Shapiro amplitude directly equals the EEC via the AdS/CFT correspondence in the strong-coupling limit."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"A precise mapping from the world-sheet integral of the AdS Virasoro-Shapiro amplitude to the energy-energy correlator in strongly coupled N=4 SYM, with explicit flat-space and first curvature correction terms."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"The world-sheet integral of the AdS Virasoro-Shapiro amplitude directly equals the energy-energy correlator in strongly coupled N=4 super Yang-Mills."}],"snapshot_sha256":"12fcc985eea6e35bec2d952f5fb5cca6b32a00cbde37f8ea31ab9a0da522529b"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We establish a precise formula relating the world-sheet integral of the AdS Virasoro-Shapiro amplitude to the energy-energy correlator (EEC) in $\\mathcal{N}=4$ super Yang-Mills theory at strong coupling. This mapping allows us to evaluate the coefficients of the AdS curvature expansion of the EEC in terms of the world-sheet integral over a unit disk. To illustrate this idea, we explicitly compute the flat-space contribution and the first curvature correction to the EEC. Our results provide a rigorous description of the stringy energy flow, demonstrating how world-sheet correlators imprint them","authors_text":"Bo Wang, Congkao Wen, Lecheng Ren","cross_cats":[],"headline":"The world-sheet integral of the AdS Virasoro-Shapiro amplitude directly equals the energy-energy correlator in strongly coupled N=4 super Yang-Mills.","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-01-08T19:00:01Z","title":"Energy-Energy Correlator from the AdS Virasoro-Shapiro Amplitude"},"references":{"count":68,"internal_anchors":17,"resolved_work":68,"sample":[{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":1,"title":"C. L. Basham, L. S. Brown, S. D. Ellis, and S. T. Love, Energy Correlations in electron - Positron Annihilation: Testing QCD, Phys. Rev. Lett.41, 1585 (1978)","work_id":"339a5aee-7c2e-4090-be91-b0b72170deaa","year":1978},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":2,"title":"C. L. Basham, L. S. Brown, S. D. Ellis, and S. T. Love, Energy Correlations in electron-Positron Annihilation in Quantum Chromodynamics: Asymptotically Free Per- turbation Theory, Phys. Rev. D19, 2018","work_id":"b5d39377-54d1-49e6-b8c7-a2e511968152","year":2018},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":3,"title":"H. Chen, I. Moult, X. Zhang, and H. X. Zhu, Rethinking jets with energy correlators: Tracks, resummation, and analytic continuation, Phys. Rev. D102, 054012 (2020), arXiv:2004.11381 [hep-ph]","work_id":"92a3b463-f7e5-4724-b677-a945c1e15119","year":2020},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":4,"title":"P. T. Komiske, I. Moult, J. Thaler, and H. X. Zhu, Analyzing N-Point Energy Correlators inside Jets with CMS Open Data, Phys. Rev. Lett.130, 051901 (2023), arXiv:2201.07800 [hep-ph]","work_id":"82770c84-1678-4493-b1fe-bd77eaef85f0","year":2023},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":5,"title":"Energy Correlators: A Journey From Theory to Experiment,","work_id":"e0b906f9-98ac-4435-b30b-e10dfb0c9afb","year":2025}],"snapshot_sha256":"a45efd67a4528e643699c0523105fbcde4e9ba7f5420bd58492c5fb1d2e54740"},"source":{"id":"2601.05312","kind":"arxiv","version":3},"verdict":{"created_at":"2026-05-16T15:45:44.402487Z","id":"183c17a0-288a-4b6a-9739-21aba6ac1b1e","model_set":{"reader":"grok-4.3"},"one_line_summary":"A precise mapping from the world-sheet integral of the AdS Virasoro-Shapiro amplitude to the energy-energy correlator in strongly coupled N=4 SYM, with explicit flat-space and first curvature correction terms.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"The world-sheet integral of the AdS Virasoro-Shapiro amplitude directly equals the energy-energy correlator in strongly coupled N=4 super Yang-Mills.","strongest_claim":"We establish a precise formula relating the world-sheet integral of the AdS Virasoro-Shapiro amplitude to the energy-energy correlator (EEC) in N=4 super Yang-Mills theory at strong coupling.","weakest_assumption":"The assumption that the world-sheet integral of the AdS Virasoro-Shapiro amplitude directly equals the EEC via the AdS/CFT correspondence in the strong-coupling limit."}},"verdict_id":"183c17a0-288a-4b6a-9739-21aba6ac1b1e"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:a1d0615e38fdc4f760b8d899aae329f489257545938fbf8fff4850a66c1a5f19","target":"record","created_at":"2026-05-18T02:45:12Z","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":"e7f28bad5b882501464e05a684d2bafd4d49e36b104ec4248a500ba33f2e7c01","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-01-08T19:00:01Z","title_canon_sha256":"a04b4fa81878d7c2c2f283e2c2cd3114653291015065d8187cab776881a1926e"},"schema_version":"1.0","source":{"id":"2601.05312","kind":"arxiv","version":3}},"canonical_sha256":"d06098d84f2b8be620629c1dbe0aeb28e541eaabe44d2ee2a67daafca49a6b2f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d06098d84f2b8be620629c1dbe0aeb28e541eaabe44d2ee2a67daafca49a6b2f","first_computed_at":"2026-05-18T02:45:12.086904Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:45:12.086904Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"A9G6gwEmkMGt8fWaN/tZeIRMHZiZ0PRztwUC4HKQOF9zpbGcwhGrruUi1xzAJWOfgUU2e127uuUZyrZnh0IhBw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:45:12.087470Z","signed_message":"canonical_sha256_bytes"},"source_id":"2601.05312","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a1d0615e38fdc4f760b8d899aae329f489257545938fbf8fff4850a66c1a5f19","sha256:3a84d34a9a9cc1dd0b1f137405e848c753ebd04bbf06d60047c88bbb82a64b14"],"state_sha256":"3f2cd8e95d89db834e62a1943bfdb77e635398d5cd6120c5c103a7f4599071e5"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XiP7nekimmLsRwgFp09Q2c/dETag9VBb6WtgbCsPsUchCJiVH+XbbgRr65PlQzyrOzkMXUbNjkxExU8pkUMBCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T04:09:49.358017Z","bundle_sha256":"b42ef92f450dea342fa7f7364ca2fd4196964913f5ff635f925491d633f69498"}}