{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:OECSLGEK7MFDTLZDDHKSCAUFAA","short_pith_number":"pith:OECSLGEK","schema_version":"1.0","canonical_sha256":"710525988afb0a39af2319d521028500147f09c741bfbf91e929435e962664ee","source":{"kind":"arxiv","id":"1310.1178","version":2},"attestation_state":"computed","paper":{"title":"Dead layer on silicon p-i-n diode charged-particle detectors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex"],"primary_cat":"physics.ins-det","authors_text":"A. Beglarian, B. A. VanDevender, B. L. Wall, D. A. Peterson, D. S. Parno, E. L. Martin, F. Harms, G. C. Harper, H. C. Bichsel, J. F. Amsbaugh, J. F. Wilkerson, J. Schwarz, K. J. Wierman, L. I. Bodine, L. Petzold, M. A. Howe, M. Steidl, N. M. Boyd, P. J. Doe, P. Renschler, R. G. H. Robertson, S. Enomoto, S. W\\\"ustling, T. Bergmann, T. D. Van Wechel, T. H. Burritt, T. J. Corona, Z. Chaoui","submitted_at":"2013-10-04T06:23:36Z","abstract_excerpt":"Semiconductor detectors in general have a dead layer at their surfaces that is either a result of natural or induced passivation, or is formed during the process of making a contact. Charged particles passing through this region produce ionization that is incompletely collected and recorded, which leads to departures from the ideal in both energy deposition and resolution. The silicon \\textit{p-i-n} diode used in the KATRIN neutrino-mass experiment has such a dead layer. We have constructed a detailed Monte Carlo model for the passage of electrons from vacuum into a silicon detector, and compa"},"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":"1310.1178","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2013-10-04T06:23:36Z","cross_cats_sorted":["hep-ex","nucl-ex"],"title_canon_sha256":"d9a402602c322d6beff091ec5d45b9c242abc0d16576d5fd25f2b6087ce83726","abstract_canon_sha256":"e33aa1be38cbec9ef90b30ea3c4819368aef81bbf3acb1b2e6afa2777ccbbb9a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:44:08.435624Z","signature_b64":"8THbdKiV0hzPSoASR6ep6foLnM+5+u8SL6AenEgN8KF3F/ycD60bP8UPhhNOKtBXvHZdzUMHm5Qt7LUssUbhCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"710525988afb0a39af2319d521028500147f09c741bfbf91e929435e962664ee","last_reissued_at":"2026-05-18T02:44:08.435171Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:44:08.435171Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dead layer on silicon p-i-n diode charged-particle detectors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex"],"primary_cat":"physics.ins-det","authors_text":"A. Beglarian, B. A. VanDevender, B. L. Wall, D. A. Peterson, D. S. Parno, E. L. Martin, F. Harms, G. C. Harper, H. C. Bichsel, J. F. Amsbaugh, J. F. Wilkerson, J. Schwarz, K. J. Wierman, L. I. Bodine, L. Petzold, M. A. Howe, M. Steidl, N. M. Boyd, P. J. Doe, P. Renschler, R. G. H. Robertson, S. Enomoto, S. W\\\"ustling, T. Bergmann, T. D. Van Wechel, T. H. Burritt, T. J. Corona, Z. Chaoui","submitted_at":"2013-10-04T06:23:36Z","abstract_excerpt":"Semiconductor detectors in general have a dead layer at their surfaces that is either a result of natural or induced passivation, or is formed during the process of making a contact. Charged particles passing through this region produce ionization that is incompletely collected and recorded, which leads to departures from the ideal in both energy deposition and resolution. The silicon \\textit{p-i-n} diode used in the KATRIN neutrino-mass experiment has such a dead layer. We have constructed a detailed Monte Carlo model for the passage of electrons from vacuum into a silicon detector, and compa"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.1178","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":""},"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":"1310.1178","created_at":"2026-05-18T02:44:08.435234+00:00"},{"alias_kind":"arxiv_version","alias_value":"1310.1178v2","created_at":"2026-05-18T02:44:08.435234+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.1178","created_at":"2026-05-18T02:44:08.435234+00:00"},{"alias_kind":"pith_short_12","alias_value":"OECSLGEK7MFD","created_at":"2026-05-18T12:27:54.935989+00:00"},{"alias_kind":"pith_short_16","alias_value":"OECSLGEK7MFDTLZD","created_at":"2026-05-18T12:27:54.935989+00:00"},{"alias_kind":"pith_short_8","alias_value":"OECSLGEK","created_at":"2026-05-18T12:27:54.935989+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/OECSLGEK7MFDTLZDDHKSCAUFAA","json":"https://pith.science/pith/OECSLGEK7MFDTLZDDHKSCAUFAA.json","graph_json":"https://pith.science/api/pith-number/OECSLGEK7MFDTLZDDHKSCAUFAA/graph.json","events_json":"https://pith.science/api/pith-number/OECSLGEK7MFDTLZDDHKSCAUFAA/events.json","paper":"https://pith.science/paper/OECSLGEK"},"agent_actions":{"view_html":"https://pith.science/pith/OECSLGEK7MFDTLZDDHKSCAUFAA","download_json":"https://pith.science/pith/OECSLGEK7MFDTLZDDHKSCAUFAA.json","view_paper":"https://pith.science/paper/OECSLGEK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1310.1178&json=true","fetch_graph":"https://pith.science/api/pith-number/OECSLGEK7MFDTLZDDHKSCAUFAA/graph.json","fetch_events":"https://pith.science/api/pith-number/OECSLGEK7MFDTLZDDHKSCAUFAA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OECSLGEK7MFDTLZDDHKSCAUFAA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OECSLGEK7MFDTLZDDHKSCAUFAA/action/storage_attestation","attest_author":"https://pith.science/pith/OECSLGEK7MFDTLZDDHKSCAUFAA/action/author_attestation","sign_citation":"https://pith.science/pith/OECSLGEK7MFDTLZDDHKSCAUFAA/action/citation_signature","submit_replication":"https://pith.science/pith/OECSLGEK7MFDTLZDDHKSCAUFAA/action/replication_record"}},"created_at":"2026-05-18T02:44:08.435234+00:00","updated_at":"2026-05-18T02:44:08.435234+00:00"}