{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:YTCNCTZGPJZJVBUZFKLKI6MIEJ","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":"7f7eb411444526feaaca798205054436833eef71ee8aee1e836bbf7293a73c7c","cross_cats_sorted":["nucl-ex"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2025-02-26T19:17:29Z","title_canon_sha256":"24fe8e52862583c67a94c641f833f42bad6a860a8897c2ccce59e8611301d87d"},"schema_version":"1.0","source":{"id":"2502.19508","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2502.19508","created_at":"2026-07-05T10:27:26Z"},{"alias_kind":"arxiv_version","alias_value":"2502.19508v2","created_at":"2026-07-05T10:27:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.19508","created_at":"2026-07-05T10:27:26Z"},{"alias_kind":"pith_short_12","alias_value":"YTCNCTZGPJZJ","created_at":"2026-07-05T10:27:26Z"},{"alias_kind":"pith_short_16","alias_value":"YTCNCTZGPJZJVBUZ","created_at":"2026-07-05T10:27:26Z"},{"alias_kind":"pith_short_8","alias_value":"YTCNCTZG","created_at":"2026-07-05T10:27:26Z"}],"graph_snapshots":[{"event_id":"sha256:2f82f8fdb9499f9ee1b1794a86cd11acfbf7f5aaf9c9f66e567bbac2395c7fc5","target":"graph","created_at":"2026-07-05T10:27:26Z","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/2502.19508/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"A series of measurements have been performed with low-energy monoenergetic neutrons to characterise cross-talk between two organic scintillator detectors. Cross-talk time-of-flight spectra and probabilities were determined for neutron energies from 1.4 to 15.5 MeV and effective scattering angles ranging from $\\sim$50{\\deg} to $\\sim$100{\\deg}. Monte-Carlo simulations incorporating both the active and inactive materials making up the detectors showed reasonable agreement with the measurements. Whilst the time-of-flight spectra were very well reproduced, the cross-talk probabilities were only in ","authors_text":"B. Carniol, B. Laurent, C. Fontbonne, D. \\'Etasse, F. Delaunay, F. M. Marqu\\'es, J. Gibelin, J. Hommet, J.-M. Fontbonne, M. P\\^arlog, M. S\\'enoville, N. A. Orr, N. de S\\'er\\'eville, N. L. Achouri, T. Mart\\'inez, X. Ledoux","cross_cats":["nucl-ex"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2025-02-26T19:17:29Z","title":"Low-energy neutron cross-talk between organic scintillator detectors"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.19508","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":"sha256:4cfdcef2d7fd1a24ab7e1c5f7519061de087d7f843df939603533267cb65842c","target":"record","created_at":"2026-07-05T10:27:26Z","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":"7f7eb411444526feaaca798205054436833eef71ee8aee1e836bbf7293a73c7c","cross_cats_sorted":["nucl-ex"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2025-02-26T19:17:29Z","title_canon_sha256":"24fe8e52862583c67a94c641f833f42bad6a860a8897c2ccce59e8611301d87d"},"schema_version":"1.0","source":{"id":"2502.19508","kind":"arxiv","version":2}},"canonical_sha256":"c4c4d14f267a729a86992a96a47988227aa9b70c7e748e510495e0b67e6654d0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c4c4d14f267a729a86992a96a47988227aa9b70c7e748e510495e0b67e6654d0","first_computed_at":"2026-07-05T10:27:26.568610Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:27:26.568610Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"rpDmVUlCi1Z7LHsT8K0hCQ5/h15xiTA3P4BdoBXhdVEW75HpfoiA38uS7QgMgS1zqhFdtj4jlPVpdmLrHqO5AQ==","signature_status":"signed_v1","signed_at":"2026-07-05T10:27:26.569182Z","signed_message":"canonical_sha256_bytes"},"source_id":"2502.19508","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4cfdcef2d7fd1a24ab7e1c5f7519061de087d7f843df939603533267cb65842c","sha256:2f82f8fdb9499f9ee1b1794a86cd11acfbf7f5aaf9c9f66e567bbac2395c7fc5"],"state_sha256":"38501d2b29904aed2cf3b29842ac6772cd09fa85ca3183c41a4e0dc6bae18c74"}