{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:PFYRTRGGL7FUXTA6HZ2RBSIID5","short_pith_number":"pith:PFYRTRGG","schema_version":"1.0","canonical_sha256":"797119c4c65fcb4bcc1e3e7510c9081f44335fe369bd1718c651537d55c19d61","source":{"kind":"arxiv","id":"1402.4943","version":1},"attestation_state":"computed","paper":{"title":"Energy measurement and fragment identification using digital signals from partially depleted Si detectors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"physics.ins-det","authors_text":"A.A.Stefanini, A.Chbihi, A.Kordyasz, A.Olmi, A.Ordine, B.Borderie, C.Maiolino, D.Gruyer, D.Santonocito, E.Bonnet, E.Rosato, E.Vient, F.Gramegna, F.Salomon, G.Ademard, G.Casini, G.Pasquali, G.Pastore, G.Poggi, G.Spadaccini, J.A.Duenas, J.D.Frankland, L.Morelli, M.Bini, M.Bruno, M.Cinausero, M.F.Rivet, M.Parlog, N.Le Neindre, O.Lopez, P.Edelbruck, R.Alba, R.Bougault, S.Barlini, S.Piantelli, S.Valdre, T.Kozik, T.Marchi, T.Twarog","submitted_at":"2014-02-20T09:57:27Z","abstract_excerpt":"A study of identification properties of a Si-Si DE-E telescope exploiting an underdepleted residual-energy detector has been performed. Five different bias voltages have been used, one corresponding to full depletion, the others associated with a depleted layer ranging from 90% to 60% of the detector thickness. Fragment identification has been performed using either the DE-E technique or Pulse Shape Analysis (PSA). Both detectors are reverse mounted: particles enter from the low field side, to enhance the PSA performance. The achieved charge and mass resolution has been quantitatively expresse"},"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":"1402.4943","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2014-02-20T09:57:27Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"4a96ce619c98d7683d6fc47d5037464110f45d6b1e7b22a4ad6762884c1cebfc","abstract_canon_sha256":"dffc398079c3a5d7672b56f8e02b670d953f9701272bacf197356a71e138dd36"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:49:38.701139Z","signature_b64":"MslyOMnGXGxdAkAeFyyxHPMT0fQ8EBFb1DCT6tizhiNm/Z6JwVyOTfeEzsc5b0IPcWpNZAXbFeQFJuHGBwJ1Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"797119c4c65fcb4bcc1e3e7510c9081f44335fe369bd1718c651537d55c19d61","last_reissued_at":"2026-05-18T02:49:38.700735Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:49:38.700735Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Energy measurement and fragment identification using digital signals from partially depleted Si detectors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"physics.ins-det","authors_text":"A.A.Stefanini, A.Chbihi, A.Kordyasz, A.Olmi, A.Ordine, B.Borderie, C.Maiolino, D.Gruyer, D.Santonocito, E.Bonnet, E.Rosato, E.Vient, F.Gramegna, F.Salomon, G.Ademard, G.Casini, G.Pasquali, G.Pastore, G.Poggi, G.Spadaccini, J.A.Duenas, J.D.Frankland, L.Morelli, M.Bini, M.Bruno, M.Cinausero, M.F.Rivet, M.Parlog, N.Le Neindre, O.Lopez, P.Edelbruck, R.Alba, R.Bougault, S.Barlini, S.Piantelli, S.Valdre, T.Kozik, T.Marchi, T.Twarog","submitted_at":"2014-02-20T09:57:27Z","abstract_excerpt":"A study of identification properties of a Si-Si DE-E telescope exploiting an underdepleted residual-energy detector has been performed. Five different bias voltages have been used, one corresponding to full depletion, the others associated with a depleted layer ranging from 90% to 60% of the detector thickness. Fragment identification has been performed using either the DE-E technique or Pulse Shape Analysis (PSA). Both detectors are reverse mounted: particles enter from the low field side, to enhance the PSA performance. The achieved charge and mass resolution has been quantitatively expresse"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.4943","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":""},"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":"1402.4943","created_at":"2026-05-18T02:49:38.700814+00:00"},{"alias_kind":"arxiv_version","alias_value":"1402.4943v1","created_at":"2026-05-18T02:49:38.700814+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.4943","created_at":"2026-05-18T02:49:38.700814+00:00"},{"alias_kind":"pith_short_12","alias_value":"PFYRTRGGL7FU","created_at":"2026-05-18T12:28:43.426989+00:00"},{"alias_kind":"pith_short_16","alias_value":"PFYRTRGGL7FUXTA6","created_at":"2026-05-18T12:28:43.426989+00:00"},{"alias_kind":"pith_short_8","alias_value":"PFYRTRGG","created_at":"2026-05-18T12:28:43.426989+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/PFYRTRGGL7FUXTA6HZ2RBSIID5","json":"https://pith.science/pith/PFYRTRGGL7FUXTA6HZ2RBSIID5.json","graph_json":"https://pith.science/api/pith-number/PFYRTRGGL7FUXTA6HZ2RBSIID5/graph.json","events_json":"https://pith.science/api/pith-number/PFYRTRGGL7FUXTA6HZ2RBSIID5/events.json","paper":"https://pith.science/paper/PFYRTRGG"},"agent_actions":{"view_html":"https://pith.science/pith/PFYRTRGGL7FUXTA6HZ2RBSIID5","download_json":"https://pith.science/pith/PFYRTRGGL7FUXTA6HZ2RBSIID5.json","view_paper":"https://pith.science/paper/PFYRTRGG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1402.4943&json=true","fetch_graph":"https://pith.science/api/pith-number/PFYRTRGGL7FUXTA6HZ2RBSIID5/graph.json","fetch_events":"https://pith.science/api/pith-number/PFYRTRGGL7FUXTA6HZ2RBSIID5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PFYRTRGGL7FUXTA6HZ2RBSIID5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PFYRTRGGL7FUXTA6HZ2RBSIID5/action/storage_attestation","attest_author":"https://pith.science/pith/PFYRTRGGL7FUXTA6HZ2RBSIID5/action/author_attestation","sign_citation":"https://pith.science/pith/PFYRTRGGL7FUXTA6HZ2RBSIID5/action/citation_signature","submit_replication":"https://pith.science/pith/PFYRTRGGL7FUXTA6HZ2RBSIID5/action/replication_record"}},"created_at":"2026-05-18T02:49:38.700814+00:00","updated_at":"2026-05-18T02:49:38.700814+00:00"}