{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:3TMJRGV3L2TNTM7TQIF3F7S7EI","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":"daa4a20aaa0d096c26691f9aebedbf5843e38d70405201ac4334b8e45e9c4f90","cross_cats_sorted":["nucl-ex"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2026-06-09T14:53:56Z","title_canon_sha256":"83127ab481671a4bd8aa1bcdae43183d1969727488788f3ee0157ab990f888bc"},"schema_version":"1.0","source":{"id":"2606.10950","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2606.10950","created_at":"2026-06-10T01:10:49Z"},{"alias_kind":"arxiv_version","alias_value":"2606.10950v1","created_at":"2026-06-10T01:10:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.10950","created_at":"2026-06-10T01:10:49Z"},{"alias_kind":"pith_short_12","alias_value":"3TMJRGV3L2TN","created_at":"2026-06-10T01:10:49Z"},{"alias_kind":"pith_short_16","alias_value":"3TMJRGV3L2TNTM7T","created_at":"2026-06-10T01:10:49Z"},{"alias_kind":"pith_short_8","alias_value":"3TMJRGV3","created_at":"2026-06-10T01:10:49Z"}],"graph_snapshots":[{"event_id":"sha256:3305e27396b6e3eb39bc1161fd43be5f77fa33d78ea81fecfd65e24d8585ca3e","target":"graph","created_at":"2026-06-10T01:10:49Z","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/2606.10950/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Neutron noise methods are used to determine kinetic parameters such as the prompt neutron decay constant, but traditional pulse-counting suffers from dead-time and pile-up at high detection rates. Recent theory shows that analysing the continuous detector current can avoid these limitations if pulse-shape effects are properly treated. This work presents a feasibility study of continuous-signal neutron noise analysis based on simulations and experiments performed at two research reactors. The stochastic model of the detector current is applied to derive Rossi- and Feynman-type formulations, and","authors_text":"Gergely Klujber, Imre P\\'azsit, Istv\\'an Barth, M\\'at\\'e Istv\\'an Boros, M\\'at\\'e Szieberth, Tsuyoshi Misawa, Yasunori Kitamura","cross_cats":["nucl-ex"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2026-06-09T14:53:56Z","title":"Feasibility demonstration of continuous signal-based neutron noise measurements by experiments and simulations"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.10950","kind":"arxiv","version":1},"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":"sha256:8f77ffdc8735f6954a3fa7849e7a0154cf519f50ac0e44587708964f4ab11838","target":"record","created_at":"2026-06-10T01:10:49Z","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":"daa4a20aaa0d096c26691f9aebedbf5843e38d70405201ac4334b8e45e9c4f90","cross_cats_sorted":["nucl-ex"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2026-06-09T14:53:56Z","title_canon_sha256":"83127ab481671a4bd8aa1bcdae43183d1969727488788f3ee0157ab990f888bc"},"schema_version":"1.0","source":{"id":"2606.10950","kind":"arxiv","version":1}},"canonical_sha256":"dcd8989abb5ea6d9b3f3820bb2fe5f22182153c1c0f0eeceb2f578c9344a77f2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"dcd8989abb5ea6d9b3f3820bb2fe5f22182153c1c0f0eeceb2f578c9344a77f2","first_computed_at":"2026-06-10T01:10:49.625127Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-10T01:10:49.625127Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"IUV21IvHL1BUIl5PZ1Smt6gpdl1moNORywnB/kcDvpRxboj9YkQeqVCFWgtBm4kq2Ghp21atu6F9zcTRM+IeCQ==","signature_status":"signed_v1","signed_at":"2026-06-10T01:10:49.626032Z","signed_message":"canonical_sha256_bytes"},"source_id":"2606.10950","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8f77ffdc8735f6954a3fa7849e7a0154cf519f50ac0e44587708964f4ab11838","sha256:3305e27396b6e3eb39bc1161fd43be5f77fa33d78ea81fecfd65e24d8585ca3e"],"state_sha256":"5501bb678dab1795d922e43d7dede619db09502bbe6b8d08ad482adea49b5712"}