{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:YIDMWG43JXKGV6BX4PKUWP5OX3","short_pith_number":"pith:YIDMWG43","schema_version":"1.0","canonical_sha256":"c206cb1b9b4dd46af837e3d54b3faebed7cc10ecda0a564d7cfe6a07f94f5794","source":{"kind":"arxiv","id":"nucl-th/0206030","version":2},"attestation_state":"computed","paper":{"title":"Signatures of Nucleon Disappearance in Large Underground Detectors","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"(2) Physics Division, Edwin Kolbe (2) ((1) Department of Physics, Knoxville, Oak Ridge), Oak Ridge National Laboratory, University of Tennessee, Yuri Kamyshkov (1)","submitted_at":"2002-06-13T18:50:42Z","abstract_excerpt":"For neutrons bound inside nuclei, baryon instability can manifest itself as a decay into undetectable particles (e.g., $\\it n \\to \\nu \\nu \\bar{\\nu} $), i.e., as a disappearance of a neutron from its nuclear state. If electric charge is conserved, a similar disappearance is impossible for a proton. The existing experimental lifetime limit for neutron disappearance is 4-7 orders of magnitude lower than the lifetime limits with detectable nucleon decay products in the final state [PDG2000]. In this paper we calculated the spectrum of nuclear de-excitations that would result from the disappearance"},"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":"nucl-th/0206030","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2002-06-13T18:50:42Z","cross_cats_sorted":[],"title_canon_sha256":"b4a8722023fb5c13c125f2d50648caae073e0733a2df1568770c9d4a81573c4a","abstract_canon_sha256":"a6088569a63322bc767d7ecd2fd592e8c03e4591a493a54d5f365c0f4f8259e2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:35:29.125839Z","signature_b64":"a1lmDjAMk6GiotpfJtgoOLk/kFqjyCTB2vUH6uwas9bW/nh70dRIcjQD5YdCIOiVhaiUFN1+ji63DskxhDroDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c206cb1b9b4dd46af837e3d54b3faebed7cc10ecda0a564d7cfe6a07f94f5794","last_reissued_at":"2026-07-04T16:35:29.125379Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:35:29.125379Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Signatures of Nucleon Disappearance in Large Underground Detectors","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"(2) Physics Division, Edwin Kolbe (2) ((1) Department of Physics, Knoxville, Oak Ridge), Oak Ridge National Laboratory, University of Tennessee, Yuri Kamyshkov (1)","submitted_at":"2002-06-13T18:50:42Z","abstract_excerpt":"For neutrons bound inside nuclei, baryon instability can manifest itself as a decay into undetectable particles (e.g., $\\it n \\to \\nu \\nu \\bar{\\nu} $), i.e., as a disappearance of a neutron from its nuclear state. If electric charge is conserved, a similar disappearance is impossible for a proton. The existing experimental lifetime limit for neutron disappearance is 4-7 orders of magnitude lower than the lifetime limits with detectable nucleon decay products in the final state [PDG2000]. In this paper we calculated the spectrum of nuclear de-excitations that would result from the disappearance"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0206030","kind":"arxiv","version":2},"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/nucl-th/0206030/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":"nucl-th/0206030","created_at":"2026-07-04T16:35:29.125442+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0206030v2","created_at":"2026-07-04T16:35:29.125442+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0206030","created_at":"2026-07-04T16:35:29.125442+00:00"},{"alias_kind":"pith_short_12","alias_value":"YIDMWG43JXKG","created_at":"2026-07-04T16:35:29.125442+00:00"},{"alias_kind":"pith_short_16","alias_value":"YIDMWG43JXKGV6BX","created_at":"2026-07-04T16:35:29.125442+00:00"},{"alias_kind":"pith_short_8","alias_value":"YIDMWG43","created_at":"2026-07-04T16:35:29.125442+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/YIDMWG43JXKGV6BX4PKUWP5OX3","json":"https://pith.science/pith/YIDMWG43JXKGV6BX4PKUWP5OX3.json","graph_json":"https://pith.science/api/pith-number/YIDMWG43JXKGV6BX4PKUWP5OX3/graph.json","events_json":"https://pith.science/api/pith-number/YIDMWG43JXKGV6BX4PKUWP5OX3/events.json","paper":"https://pith.science/paper/YIDMWG43"},"agent_actions":{"view_html":"https://pith.science/pith/YIDMWG43JXKGV6BX4PKUWP5OX3","download_json":"https://pith.science/pith/YIDMWG43JXKGV6BX4PKUWP5OX3.json","view_paper":"https://pith.science/paper/YIDMWG43","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/0206030&json=true","fetch_graph":"https://pith.science/api/pith-number/YIDMWG43JXKGV6BX4PKUWP5OX3/graph.json","fetch_events":"https://pith.science/api/pith-number/YIDMWG43JXKGV6BX4PKUWP5OX3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YIDMWG43JXKGV6BX4PKUWP5OX3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YIDMWG43JXKGV6BX4PKUWP5OX3/action/storage_attestation","attest_author":"https://pith.science/pith/YIDMWG43JXKGV6BX4PKUWP5OX3/action/author_attestation","sign_citation":"https://pith.science/pith/YIDMWG43JXKGV6BX4PKUWP5OX3/action/citation_signature","submit_replication":"https://pith.science/pith/YIDMWG43JXKGV6BX4PKUWP5OX3/action/replication_record"}},"created_at":"2026-07-04T16:35:29.125442+00:00","updated_at":"2026-07-04T16:35:29.125442+00:00"}