{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:YA5KZOFALOIAPBH3Z4JHY6LFLZ","short_pith_number":"pith:YA5KZOFA","schema_version":"1.0","canonical_sha256":"c03aacb8a05b900784fbcf127c79655e6b1ff807abbc2add9816024c01152679","source":{"kind":"arxiv","id":"2303.10507","version":1},"attestation_state":"computed","paper":{"title":"A search for neutron-to-hidden-neutron oscillations in a ultra-cold neutron beam","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"B. Cl\\'ement, B. Perriolat, G. Ban, G. Pignol, J. Chen, M. Guigue, O. Naviliat-Cuncic, P.-J. Chiu, P. Larue, P. Schmidt-Wellenburg, S. Roccia, T. Jenke, T. Lefort, W. Saenz-Arevalo","submitted_at":"2023-03-18T21:58:05Z","abstract_excerpt":"Models that postulate the existence of hidden sectors address contemporary questions, such as the source of baryogenesis and the nature of dark matter. Among the possible mixing processes, neutron-to-hidden-neutron oscillations have been repeatedly tested with ultra-cold neutron storage and passing-through-wall experiments in the range of small ($\\delta m<2$ peV) and large mass splitting ($\\delta m>10$ neV), respectively. In this work, we present a new constraint in the oscillation parameter space derived from neutron disappearance in ultra-cold neutron beam experiments. The overall limit, whi"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2303.10507","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"hep-ph","submitted_at":"2023-03-18T21:58:05Z","cross_cats_sorted":[],"title_canon_sha256":"cbd0bfe4966b19217edd105aa5dca07ca778f215b036fb90c5e4fa9c3e8ffd7f","abstract_canon_sha256":"2cf0dcd5c0998ef37c2b09afbdd56266b00b3e45cb5086a7a7dcc9328f25ec07"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:11:54.777597Z","signature_b64":"JuTo2MYFC01PVEAvb1XWFIJi/oZ51sMZkiOlLuuIetOLA80w81lVsWrpKT27VKqARgRUN6Av9gPmOFz1RpN+BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c03aacb8a05b900784fbcf127c79655e6b1ff807abbc2add9816024c01152679","last_reissued_at":"2026-07-05T07:11:54.777145Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:11:54.777145Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A search for neutron-to-hidden-neutron oscillations in a ultra-cold neutron beam","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"B. Cl\\'ement, B. Perriolat, G. Ban, G. Pignol, J. Chen, M. Guigue, O. Naviliat-Cuncic, P.-J. Chiu, P. Larue, P. Schmidt-Wellenburg, S. Roccia, T. Jenke, T. Lefort, W. Saenz-Arevalo","submitted_at":"2023-03-18T21:58:05Z","abstract_excerpt":"Models that postulate the existence of hidden sectors address contemporary questions, such as the source of baryogenesis and the nature of dark matter. Among the possible mixing processes, neutron-to-hidden-neutron oscillations have been repeatedly tested with ultra-cold neutron storage and passing-through-wall experiments in the range of small ($\\delta m<2$ peV) and large mass splitting ($\\delta m>10$ neV), respectively. In this work, we present a new constraint in the oscillation parameter space derived from neutron disappearance in ultra-cold neutron beam experiments. The overall limit, whi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2303.10507","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2303.10507/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2303.10507","created_at":"2026-07-05T07:11:54.777202+00:00"},{"alias_kind":"arxiv_version","alias_value":"2303.10507v1","created_at":"2026-07-05T07:11:54.777202+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2303.10507","created_at":"2026-07-05T07:11:54.777202+00:00"},{"alias_kind":"pith_short_12","alias_value":"YA5KZOFALOIA","created_at":"2026-07-05T07:11:54.777202+00:00"},{"alias_kind":"pith_short_16","alias_value":"YA5KZOFALOIAPBH3","created_at":"2026-07-05T07:11:54.777202+00:00"},{"alias_kind":"pith_short_8","alias_value":"YA5KZOFA","created_at":"2026-07-05T07:11:54.777202+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/YA5KZOFALOIAPBH3Z4JHY6LFLZ","json":"https://pith.science/pith/YA5KZOFALOIAPBH3Z4JHY6LFLZ.json","graph_json":"https://pith.science/api/pith-number/YA5KZOFALOIAPBH3Z4JHY6LFLZ/graph.json","events_json":"https://pith.science/api/pith-number/YA5KZOFALOIAPBH3Z4JHY6LFLZ/events.json","paper":"https://pith.science/paper/YA5KZOFA"},"agent_actions":{"view_html":"https://pith.science/pith/YA5KZOFALOIAPBH3Z4JHY6LFLZ","download_json":"https://pith.science/pith/YA5KZOFALOIAPBH3Z4JHY6LFLZ.json","view_paper":"https://pith.science/paper/YA5KZOFA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2303.10507&json=true","fetch_graph":"https://pith.science/api/pith-number/YA5KZOFALOIAPBH3Z4JHY6LFLZ/graph.json","fetch_events":"https://pith.science/api/pith-number/YA5KZOFALOIAPBH3Z4JHY6LFLZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YA5KZOFALOIAPBH3Z4JHY6LFLZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YA5KZOFALOIAPBH3Z4JHY6LFLZ/action/storage_attestation","attest_author":"https://pith.science/pith/YA5KZOFALOIAPBH3Z4JHY6LFLZ/action/author_attestation","sign_citation":"https://pith.science/pith/YA5KZOFALOIAPBH3Z4JHY6LFLZ/action/citation_signature","submit_replication":"https://pith.science/pith/YA5KZOFALOIAPBH3Z4JHY6LFLZ/action/replication_record"}},"created_at":"2026-07-05T07:11:54.777202+00:00","updated_at":"2026-07-05T07:11:54.777202+00:00"}