{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:HGGE5COLTGC3DOPW5SWJ2XQJGR","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":"b1007baa49ef9cf7f54ecdab6cc4890498c6b1c73cd7fe03715a4c59b7ef32d7","cross_cats_sorted":["hep-ex","nucl-ex"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2024-11-18T18:18:43Z","title_canon_sha256":"238507b82187a20ca0f5f65efb2b4d6b19dd742e86b08d76737026bd4aac6954"},"schema_version":"1.0","source":{"id":"2411.11804","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2411.11804","created_at":"2026-07-05T12:01:19Z"},{"alias_kind":"arxiv_version","alias_value":"2411.11804v2","created_at":"2026-07-05T12:01:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.11804","created_at":"2026-07-05T12:01:19Z"},{"alias_kind":"pith_short_12","alias_value":"HGGE5COLTGC3","created_at":"2026-07-05T12:01:19Z"},{"alias_kind":"pith_short_16","alias_value":"HGGE5COLTGC3DOPW","created_at":"2026-07-05T12:01:19Z"},{"alias_kind":"pith_short_8","alias_value":"HGGE5COL","created_at":"2026-07-05T12:01:19Z"}],"graph_snapshots":[{"event_id":"sha256:77d31ef198e2d0329e11dbb9933da03d73ddae53473b74ccf4282affc7270543","target":"graph","created_at":"2026-07-05T12:01:19Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2411.11804/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"There is a growing realization that neutrinos can be used as a diagnostic tool to better understand the inner workings of a nuclear weapon. Robust estimates demonstrate that an Inverse Beta Decay (IBD) neutrino scintillation detector built at the Nevada Test Site of 1000-ton active target mass at a standoff distance of 500 m would detect thousands of neutrino events per kTe of nuclear yield. This would provide less than 4% statistical error on measured neutrino rate and 5% error on neutrino energy. Extrapolating this to an error on the test device explosive yield requires knowledge from evalua","authors_text":"A.C. Hayes, B.T. Turner, E.C. Dunton, G.W. Misch, J.D. Martin, J.M. Durham, J.R. Distel, M.R. Mumpower, R.G. Van de Water, R.T. Thornton, W.C. Louis, W.S. Wilburn, Z. Tang","cross_cats":["hep-ex","nucl-ex"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2024-11-18T18:18:43Z","title":"Novel Application of Neutrinos to Evaluate U.S. Nuclear Weapons Performance"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.11804","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:f69e7638c415dc21692de81f91f9fc8d3e72fdc1520d5aa7f4fe9070f592a418","target":"record","created_at":"2026-07-05T12:01:19Z","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":"b1007baa49ef9cf7f54ecdab6cc4890498c6b1c73cd7fe03715a4c59b7ef32d7","cross_cats_sorted":["hep-ex","nucl-ex"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2024-11-18T18:18:43Z","title_canon_sha256":"238507b82187a20ca0f5f65efb2b4d6b19dd742e86b08d76737026bd4aac6954"},"schema_version":"1.0","source":{"id":"2411.11804","kind":"arxiv","version":2}},"canonical_sha256":"398c4e89cb9985b1b9f6ecac9d5e093458b5b716c05f175f002ff5896cc41af6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"398c4e89cb9985b1b9f6ecac9d5e093458b5b716c05f175f002ff5896cc41af6","first_computed_at":"2026-07-05T12:01:19.881841Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T12:01:19.881841Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"IxHQKGG96z2DvwspGOIHxvp4Zle3BHmI7ZF8Zy4Xm+heJ3s6JXMsGS3C6gj+kR3ZwuxIcQKvq9xr5Y45Df49Aw==","signature_status":"signed_v1","signed_at":"2026-07-05T12:01:19.882397Z","signed_message":"canonical_sha256_bytes"},"source_id":"2411.11804","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f69e7638c415dc21692de81f91f9fc8d3e72fdc1520d5aa7f4fe9070f592a418","sha256:77d31ef198e2d0329e11dbb9933da03d73ddae53473b74ccf4282affc7270543"],"state_sha256":"57d2893ede738a2ef49576d17fdc0cbbbaf3f12268ddc2830f4d81c20552efe8"}