{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:NL7SAU4N2BN6SONKLDXS2YA7PQ","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":"a5f00787d1f039f9e781fca5e95b5b2c240038f2bad066948fda23617cba117b","cross_cats_sorted":["nucl-ex"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2026-05-25T10:19:35Z","title_canon_sha256":"02c4465ac552131531636c94e26b143af27fafeb24a3c850b2187bd4724380c7"},"schema_version":"1.0","source":{"id":"2606.02613","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2606.02613","created_at":"2026-06-03T00:05:04Z"},{"alias_kind":"arxiv_version","alias_value":"2606.02613v1","created_at":"2026-06-03T00:05:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.02613","created_at":"2026-06-03T00:05:04Z"},{"alias_kind":"pith_short_12","alias_value":"NL7SAU4N2BN6","created_at":"2026-06-03T00:05:04Z"},{"alias_kind":"pith_short_16","alias_value":"NL7SAU4N2BN6SONK","created_at":"2026-06-03T00:05:04Z"},{"alias_kind":"pith_short_8","alias_value":"NL7SAU4N","created_at":"2026-06-03T00:05:04Z"}],"graph_snapshots":[{"event_id":"sha256:d26f957ed34916546de713afd0f098e389b77d90cb3c332af936c46e24114522","target":"graph","created_at":"2026-06-03T00:05:04Z","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/2606.02613/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The discrimination of neutron and gamma pulse shapes is a key technology in fields such as nuclear safety monitoring and radiation assessment. An enhanced recursive gated cyclic residual-sparse linear attention network is developed on the CLYC detector experimental platform to overcome weak noise resistance, limited feature extraction and inferior real-time performance of conventional algorithms. The experimental dataset comprises 19,971 samples, which were pre-processed and stratified for model training and testing. Results indicate that the proposed algorithm achieves a quality factor of 2.2","authors_text":"Fuquan Jia, Guofeng Qu, Hailong Xu, Jia Song, Shengduo Liu, Shiwei Jing, Sijia Zhou, Siqi Liu, Tian Zhang, Weiyang Zhang, Yue Sun, Yuxuan Gu, Zebin Li, Zhihua Gao","cross_cats":["nucl-ex"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2026-05-25T10:19:35Z","title":"A Method for Neutron-Gamma Pulse Shape Discrimination of CLYC Detector Based on a Gated Residual-Linear Attention Network"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.02613","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:a674c22253d901e0f5312f1f4f8cf79255b66383589bf9ffbd74962895e73ba0","target":"record","created_at":"2026-06-03T00:05:04Z","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":"a5f00787d1f039f9e781fca5e95b5b2c240038f2bad066948fda23617cba117b","cross_cats_sorted":["nucl-ex"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2026-05-25T10:19:35Z","title_canon_sha256":"02c4465ac552131531636c94e26b143af27fafeb24a3c850b2187bd4724380c7"},"schema_version":"1.0","source":{"id":"2606.02613","kind":"arxiv","version":1}},"canonical_sha256":"6aff20538dd05be939aa58ef2d601f7c06dd4b33ae9bea785fdfcd66036bcf17","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6aff20538dd05be939aa58ef2d601f7c06dd4b33ae9bea785fdfcd66036bcf17","first_computed_at":"2026-06-03T00:05:04.628985Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-03T00:05:04.628985Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"G/8BPQflHhwNjDIA0bWFy7XusXk+GL642VO3joU7ILZh38RCsoQPWPugOnOnTEKWQlxB1NKPAXu9WPLsc3epCA==","signature_status":"signed_v1","signed_at":"2026-06-03T00:05:04.629390Z","signed_message":"canonical_sha256_bytes"},"source_id":"2606.02613","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a674c22253d901e0f5312f1f4f8cf79255b66383589bf9ffbd74962895e73ba0","sha256:d26f957ed34916546de713afd0f098e389b77d90cb3c332af936c46e24114522"],"state_sha256":"22dcfd07f307d2dcafa736bd22492f9f3b5cd95e09df67f8004b0ffda32d055d"}