{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:A4VI6DSEBGF6IJJNYBRNLCY3PQ","short_pith_number":"pith:A4VI6DSE","canonical_record":{"source":{"id":"1007.1727","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.data-an","submitted_at":"2010-07-10T15:48:35Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"bb711af71e2871faa3fc91c24c889cb280a990ac424b3e916d3b09544a4fee8d","abstract_canon_sha256":"16a2eea541e7db7939ec01439778e9623842fcb5e5c033026e0de4c7d64e18a4"},"schema_version":"1.0"},"canonical_sha256":"072a8f0e44098be4252dc062d58b1b7c160fe511fe5732255255923c6ec430ff","source":{"kind":"arxiv","id":"1007.1727","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1007.1727","created_at":"2026-07-04T18:34:18Z"},{"alias_kind":"arxiv_version","alias_value":"1007.1727v3","created_at":"2026-07-04T18:34:18Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1007.1727","created_at":"2026-07-04T18:34:18Z"},{"alias_kind":"pith_short_12","alias_value":"A4VI6DSEBGF6","created_at":"2026-07-04T18:34:18Z"},{"alias_kind":"pith_short_16","alias_value":"A4VI6DSEBGF6IJJN","created_at":"2026-07-04T18:34:18Z"},{"alias_kind":"pith_short_8","alias_value":"A4VI6DSE","created_at":"2026-07-04T18:34:18Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:A4VI6DSEBGF6IJJNYBRNLCY3PQ","target":"record","payload":{"canonical_record":{"source":{"id":"1007.1727","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.data-an","submitted_at":"2010-07-10T15:48:35Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"bb711af71e2871faa3fc91c24c889cb280a990ac424b3e916d3b09544a4fee8d","abstract_canon_sha256":"16a2eea541e7db7939ec01439778e9623842fcb5e5c033026e0de4c7d64e18a4"},"schema_version":"1.0"},"canonical_sha256":"072a8f0e44098be4252dc062d58b1b7c160fe511fe5732255255923c6ec430ff","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T18:34:18.549862Z","signature_b64":"f8V/nbMTgM2J0uhY/SO2zPK0caNVTBCab1KrgNiDvYWIZKSMWZoL6eUgRKLqAzfAZ8cXKbxxp3/+PSTeC9/mDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"072a8f0e44098be4252dc062d58b1b7c160fe511fe5732255255923c6ec430ff","last_reissued_at":"2026-07-04T18:34:18.549349Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T18:34:18.549349Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1007.1727","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":"2026-07-04T18:34:18Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LNzmuzwWtmqd8CG1DizYc1T60els832TKamqYxtn8K6UZJzY+J0ibfh426g6yltU+gsGkCxqriTDoDdMuyJICg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-17T14:06:01.419383Z"},"content_sha256":"7bdf2128e79a05bdbad3e39847c59ba6a714c7c861a10deb56cf004cedbf32c3","schema_version":"1.0","event_id":"sha256:7bdf2128e79a05bdbad3e39847c59ba6a714c7c861a10deb56cf004cedbf32c3"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:A4VI6DSEBGF6IJJNYBRNLCY3PQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Asymptotic formulae for likelihood-based tests of new physics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"Explicit asymptotic formulae are derived for the distributions of likelihood ratio test statistics in searches for new physics, including systematic uncertainties, along with the Asimov dataset for computing median experimental sensitivity.","cross_cats":["hep-ex"],"primary_cat":"physics.data-an","authors_text":"Eilam Gross, Glen Cowan, Kyle Cranmer, Ofer Vitells","submitted_at":"2010-07-10T15:48:35Z","abstract_excerpt":"We describe likelihood-based statistical tests for use in high energy physics for the discovery of new phenomena and for construction of confidence intervals on model parameters. We focus on the properties of the test procedures that allow one to account for systematic uncertainties. Explicit formulae for the asymptotic distributions of test statistics are derived using results of Wilks and Wald. We motivate and justify the use of a representative data set, called the \"Asimov data set\", which provides a simple method to obtain the median experimental sensitivity of a search or measurement as w"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"We derive explicit formulae for the asymptotic distributions of test statistics... We motivate and justify the use of a representative data set, called the 'Asimov data set', which provides a simple method to obtain the median experimental sensitivity of a search or measurement.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"The regularity conditions of Wilks' and Wald's theorems hold for the profiled likelihood (large sample size, interior maximum, differentiable likelihood), which the paper invokes without deriving or testing the boundary cases that arise when signal strength is constrained to be non-negative.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"Asymptotic distributions of profiled likelihood-ratio test statistics are derived for new-physics searches and parameter estimation, with the Asimov dataset supplying a direct route to median experimental sensitivity.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"Explicit asymptotic formulae are derived for the distributions of likelihood ratio test statistics in searches for new physics, including systematic uncertainties, along with the Asimov dataset for computing median experimental sensitivity.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"e9715ebab0d12aa86b50606b97a90b36fc6b5b6def392df3a9d9c0ff75bd5594"},"source":{"id":"1007.1727","kind":"arxiv","version":3},"verdict":{"id":"68f68c96-45bf-408e-ac41-86a67f58d211","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-11T01:44:37.886555Z","strongest_claim":"We derive explicit formulae for the asymptotic distributions of test statistics... We motivate and justify the use of a representative data set, called the 'Asimov data set', which provides a simple method to obtain the median experimental sensitivity of a search or measurement.","one_line_summary":"Asymptotic distributions of profiled likelihood-ratio test statistics are derived for new-physics searches and parameter estimation, with the Asimov dataset supplying a direct route to median experimental sensitivity.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"The regularity conditions of Wilks' and Wald's theorems hold for the profiled likelihood (large sample size, interior maximum, differentiable likelihood), which the paper invokes without deriving or testing the boundary cases that arise when signal strength is constrained to be non-negative.","pith_extraction_headline":"Explicit asymptotic formulae are derived for the distributions of likelihood ratio test statistics in searches for new physics, including systematic uncertainties, along with the Asimov dataset for computing median experimental sensitivity."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1007.1727/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":18,"sample":[{"doi":"","year":1938,"title":"Wilks, The large-sample distribution of the likelihood ratio for te sting composite hypotheses, Ann","work_id":"61c984aa-77ad-4666-a705-b166aab07558","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":1943,"title":"Wald, Tests of Statistical Hypotheses Concerning Several Paramet ers When the Number of Observations is Large , Transactions of the American Mathematical Society, Vol","work_id":"b1677685-fdfb-41ab-9799-e2970dba074b","ref_index":2,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":1990,"title":"1 , Broadway Books","work_id":"1698e488-3b8c-422f-b9e1-f808d52cc56e","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2005,"title":"V. Bartsch and G. Quast, Expected signal observability at future experiments , CMS Note 2005/004 (2003) (available on CMS information server)","work_id":"d8b1e3a8-db34-4243-9cf2-c00a5b95ad5d","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2008,"title":"ATLAS Collaboration, Expected Performance of the ATLAS Experiment, Detector, Trigger and Physics , CERN-OPEN-2008-020, Geneva, 2008, e-print: arXiv:0901. 0512","work_id":"3c9e7b8a-ccc6-4fde-aef6-facb649e478e","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":18,"snapshot_sha256":"eeebc4dd003ccb5bb38a135e69dfc75fdc2ff76217b64782d400af199e025e42","internal_anchors":1},"formal_canon":{"evidence_count":2,"snapshot_sha256":"54e67eae6e4d480e628ccf422be56a9cfc7e0a7167c3efd280c969a278a790dd"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":"68f68c96-45bf-408e-ac41-86a67f58d211"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T18:34:18Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ldG/g2dgvL08+n0MJPW68xufpM5mJ6tgCeVYoqVTQnaFoJ+Ukc9L5bgrS60NYL7W4WlVAMP7BiCeIld712KxAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-17T14:06:01.420071Z"},"content_sha256":"43aa2238ff9aa67df6bd217d697d01a72a7a66410689fad49f8ab2e5e012d374","schema_version":"1.0","event_id":"sha256:43aa2238ff9aa67df6bd217d697d01a72a7a66410689fad49f8ab2e5e012d374"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/A4VI6DSEBGF6IJJNYBRNLCY3PQ/bundle.json","state_url":"https://pith.science/pith/A4VI6DSEBGF6IJJNYBRNLCY3PQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/A4VI6DSEBGF6IJJNYBRNLCY3PQ/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":"2026-08-17T14:06:01Z","links":{"resolver":"https://pith.science/pith/A4VI6DSEBGF6IJJNYBRNLCY3PQ","bundle":"https://pith.science/pith/A4VI6DSEBGF6IJJNYBRNLCY3PQ/bundle.json","state":"https://pith.science/pith/A4VI6DSEBGF6IJJNYBRNLCY3PQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/A4VI6DSEBGF6IJJNYBRNLCY3PQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:A4VI6DSEBGF6IJJNYBRNLCY3PQ","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":"16a2eea541e7db7939ec01439778e9623842fcb5e5c033026e0de4c7d64e18a4","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.data-an","submitted_at":"2010-07-10T15:48:35Z","title_canon_sha256":"bb711af71e2871faa3fc91c24c889cb280a990ac424b3e916d3b09544a4fee8d"},"schema_version":"1.0","source":{"id":"1007.1727","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1007.1727","created_at":"2026-07-04T18:34:18Z"},{"alias_kind":"arxiv_version","alias_value":"1007.1727v3","created_at":"2026-07-04T18:34:18Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1007.1727","created_at":"2026-07-04T18:34:18Z"},{"alias_kind":"pith_short_12","alias_value":"A4VI6DSEBGF6","created_at":"2026-07-04T18:34:18Z"},{"alias_kind":"pith_short_16","alias_value":"A4VI6DSEBGF6IJJN","created_at":"2026-07-04T18:34:18Z"},{"alias_kind":"pith_short_8","alias_value":"A4VI6DSE","created_at":"2026-07-04T18:34:18Z"}],"graph_snapshots":[{"event_id":"sha256:43aa2238ff9aa67df6bd217d697d01a72a7a66410689fad49f8ab2e5e012d374","target":"graph","created_at":"2026-07-04T18:34:18Z","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 derive explicit formulae for the asymptotic distributions of test statistics... We motivate and justify the use of a representative data set, called the 'Asimov data set', which provides a simple method to obtain the median experimental sensitivity of a search or measurement."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"The regularity conditions of Wilks' and Wald's theorems hold for the profiled likelihood (large sample size, interior maximum, differentiable likelihood), which the paper invokes without deriving or testing the boundary cases that arise when signal strength is constrained to be non-negative."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"Asymptotic distributions of profiled likelihood-ratio test statistics are derived for new-physics searches and parameter estimation, with the Asimov dataset supplying a direct route to median experimental sensitivity."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"Explicit asymptotic formulae are derived for the distributions of likelihood ratio test statistics in searches for new physics, including systematic uncertainties, along with the Asimov dataset for computing median experimental sensitivity."}],"snapshot_sha256":"e9715ebab0d12aa86b50606b97a90b36fc6b5b6def392df3a9d9c0ff75bd5594"},"formal_canon":{"evidence_count":2,"snapshot_sha256":"54e67eae6e4d480e628ccf422be56a9cfc7e0a7167c3efd280c969a278a790dd"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/1007.1727/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We describe likelihood-based statistical tests for use in high energy physics for the discovery of new phenomena and for construction of confidence intervals on model parameters. We focus on the properties of the test procedures that allow one to account for systematic uncertainties. Explicit formulae for the asymptotic distributions of test statistics are derived using results of Wilks and Wald. We motivate and justify the use of a representative data set, called the \"Asimov data set\", which provides a simple method to obtain the median experimental sensitivity of a search or measurement as w","authors_text":"Eilam Gross, Glen Cowan, Kyle Cranmer, Ofer Vitells","cross_cats":["hep-ex"],"headline":"Explicit asymptotic formulae are derived for the distributions of likelihood ratio test statistics in searches for new physics, including systematic uncertainties, along with the Asimov dataset for computing median experimental sensitivity.","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.data-an","submitted_at":"2010-07-10T15:48:35Z","title":"Asymptotic formulae for likelihood-based tests of new physics"},"references":{"count":18,"internal_anchors":1,"resolved_work":18,"sample":[{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":1,"title":"Wilks, The large-sample distribution of the likelihood ratio for te sting composite hypotheses, Ann","work_id":"61c984aa-77ad-4666-a705-b166aab07558","year":1938},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":2,"title":"Wald, Tests of Statistical Hypotheses Concerning Several Paramet ers When the Number of Observations is Large , Transactions of the American Mathematical Society, Vol","work_id":"b1677685-fdfb-41ab-9799-e2970dba074b","year":1943},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":3,"title":"1 , Broadway Books","work_id":"1698e488-3b8c-422f-b9e1-f808d52cc56e","year":1990},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":4,"title":"V. Bartsch and G. Quast, Expected signal observability at future experiments , CMS Note 2005/004 (2003) (available on CMS information server)","work_id":"d8b1e3a8-db34-4243-9cf2-c00a5b95ad5d","year":2005},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":5,"title":"ATLAS Collaboration, Expected Performance of the ATLAS Experiment, Detector, Trigger and Physics , CERN-OPEN-2008-020, Geneva, 2008, e-print: arXiv:0901. 0512","work_id":"3c9e7b8a-ccc6-4fde-aef6-facb649e478e","year":2008}],"snapshot_sha256":"eeebc4dd003ccb5bb38a135e69dfc75fdc2ff76217b64782d400af199e025e42"},"source":{"id":"1007.1727","kind":"arxiv","version":3},"verdict":{"created_at":"2026-05-11T01:44:37.886555Z","id":"68f68c96-45bf-408e-ac41-86a67f58d211","model_set":{"reader":"grok-4.3"},"one_line_summary":"Asymptotic distributions of profiled likelihood-ratio test statistics are derived for new-physics searches and parameter estimation, with the Asimov dataset supplying a direct route to median experimental sensitivity.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"Explicit asymptotic formulae are derived for the distributions of likelihood ratio test statistics in searches for new physics, including systematic uncertainties, along with the Asimov dataset for computing median experimental sensitivity.","strongest_claim":"We derive explicit formulae for the asymptotic distributions of test statistics... We motivate and justify the use of a representative data set, called the 'Asimov data set', which provides a simple method to obtain the median experimental sensitivity of a search or measurement.","weakest_assumption":"The regularity conditions of Wilks' and Wald's theorems hold for the profiled likelihood (large sample size, interior maximum, differentiable likelihood), which the paper invokes without deriving or testing the boundary cases that arise when signal strength is constrained to be non-negative."}},"verdict_id":"68f68c96-45bf-408e-ac41-86a67f58d211"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:7bdf2128e79a05bdbad3e39847c59ba6a714c7c861a10deb56cf004cedbf32c3","target":"record","created_at":"2026-07-04T18:34:18Z","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":"16a2eea541e7db7939ec01439778e9623842fcb5e5c033026e0de4c7d64e18a4","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.data-an","submitted_at":"2010-07-10T15:48:35Z","title_canon_sha256":"bb711af71e2871faa3fc91c24c889cb280a990ac424b3e916d3b09544a4fee8d"},"schema_version":"1.0","source":{"id":"1007.1727","kind":"arxiv","version":3}},"canonical_sha256":"072a8f0e44098be4252dc062d58b1b7c160fe511fe5732255255923c6ec430ff","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"072a8f0e44098be4252dc062d58b1b7c160fe511fe5732255255923c6ec430ff","first_computed_at":"2026-07-04T18:34:18.549349Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T18:34:18.549349Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"f8V/nbMTgM2J0uhY/SO2zPK0caNVTBCab1KrgNiDvYWIZKSMWZoL6eUgRKLqAzfAZ8cXKbxxp3/+PSTeC9/mDw==","signature_status":"signed_v1","signed_at":"2026-07-04T18:34:18.549862Z","signed_message":"canonical_sha256_bytes"},"source_id":"1007.1727","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7bdf2128e79a05bdbad3e39847c59ba6a714c7c861a10deb56cf004cedbf32c3","sha256:43aa2238ff9aa67df6bd217d697d01a72a7a66410689fad49f8ab2e5e012d374"],"state_sha256":"48851cbbcdc499a26e3678bb70bef8254f1f25b34f4e79d641c9d92d82112b5c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iBBd/zp2SJ0LxA3IuYm8OMnC0nlzGeryJDPFN/ZPDXV9xywE2ITgGeehchiVSqqnHjjGHUpJnSkyJruknFKpDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-17T14:06:01.423913Z","bundle_sha256":"ef56cebf98ed4e6a91b3a1fc75a4005fdc49330ce063bc31abefcf596f6347c3"}}