{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:IRVF4PAE4MV4EOEL4ZFTYM7Y45","short_pith_number":"pith:IRVF4PAE","schema_version":"1.0","canonical_sha256":"446a5e3c04e32bc2388be64b3c33f8e76ec7323db0e3c66a8d9a4aae740a1d06","source":{"kind":"arxiv","id":"2010.13427","version":1},"attestation_state":"computed","paper":{"title":"Machine Learning aided 3D-position reconstruction in large LaCl$_{3}$ crystals","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.ins-det","authors_text":"C. Domingo-Pardo, D. Calvo, I. Ladarescu, J. Balibrea-Correa, J. Lerendegui-Marco, L. Caballero, P. Olleros-Rodriguez, V. Babiano","submitted_at":"2020-10-26T08:53:31Z","abstract_excerpt":"We investigate five different models to reconstruct the 3D $\\gamma$-ray hit coordinates in five large \\lacls monolithic crystals optically coupled to pixelated silicon photomultipliers. These scintillators have a base surface of 50 $\\times$ 50 mm$^2$ and five different thicknesses, from 10 mm to 30 mm. Four of these models are analytical prescriptions and one is based on a Convolutional Neural Network. Average resolutions close to 1-2mm fwhm are obtained in the transverse crystal plane for crystal thicknesses between 10 mm and 20 mm using analytical models. For thicker crystals average resolut"},"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":"2010.13427","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"physics.ins-det","submitted_at":"2020-10-26T08:53:31Z","cross_cats_sorted":[],"title_canon_sha256":"ba9e5e21b13638ae5ffc88013e9407f597e1b1280b9813038bbef9015b22eebb","abstract_canon_sha256":"c5dd0b92479acb6c3287b1d4e883d097c664c56579c5565dae7197f072158249"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:31:44.247949Z","signature_b64":"G/Q3jh/3uNjEM/049ZzMe0oScXcZwm89+5wyxOcI8FcjRdrkQeiT+HcoRX4Lje7tMYxwXz3q1cZdySEKZKpKAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"446a5e3c04e32bc2388be64b3c33f8e76ec7323db0e3c66a8d9a4aae740a1d06","last_reissued_at":"2026-07-05T02:31:44.247460Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:31:44.247460Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Machine Learning aided 3D-position reconstruction in large LaCl$_{3}$ crystals","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.ins-det","authors_text":"C. Domingo-Pardo, D. Calvo, I. Ladarescu, J. Balibrea-Correa, J. Lerendegui-Marco, L. Caballero, P. Olleros-Rodriguez, V. Babiano","submitted_at":"2020-10-26T08:53:31Z","abstract_excerpt":"We investigate five different models to reconstruct the 3D $\\gamma$-ray hit coordinates in five large \\lacls monolithic crystals optically coupled to pixelated silicon photomultipliers. These scintillators have a base surface of 50 $\\times$ 50 mm$^2$ and five different thicknesses, from 10 mm to 30 mm. Four of these models are analytical prescriptions and one is based on a Convolutional Neural Network. Average resolutions close to 1-2mm fwhm are obtained in the transverse crystal plane for crystal thicknesses between 10 mm and 20 mm using analytical models. For thicker crystals average resolut"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2010.13427","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/2010.13427/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":"2010.13427","created_at":"2026-07-05T02:31:44.247521+00:00"},{"alias_kind":"arxiv_version","alias_value":"2010.13427v1","created_at":"2026-07-05T02:31:44.247521+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2010.13427","created_at":"2026-07-05T02:31:44.247521+00:00"},{"alias_kind":"pith_short_12","alias_value":"IRVF4PAE4MV4","created_at":"2026-07-05T02:31:44.247521+00:00"},{"alias_kind":"pith_short_16","alias_value":"IRVF4PAE4MV4EOEL","created_at":"2026-07-05T02:31:44.247521+00:00"},{"alias_kind":"pith_short_8","alias_value":"IRVF4PAE","created_at":"2026-07-05T02:31:44.247521+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/IRVF4PAE4MV4EOEL4ZFTYM7Y45","json":"https://pith.science/pith/IRVF4PAE4MV4EOEL4ZFTYM7Y45.json","graph_json":"https://pith.science/api/pith-number/IRVF4PAE4MV4EOEL4ZFTYM7Y45/graph.json","events_json":"https://pith.science/api/pith-number/IRVF4PAE4MV4EOEL4ZFTYM7Y45/events.json","paper":"https://pith.science/paper/IRVF4PAE"},"agent_actions":{"view_html":"https://pith.science/pith/IRVF4PAE4MV4EOEL4ZFTYM7Y45","download_json":"https://pith.science/pith/IRVF4PAE4MV4EOEL4ZFTYM7Y45.json","view_paper":"https://pith.science/paper/IRVF4PAE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2010.13427&json=true","fetch_graph":"https://pith.science/api/pith-number/IRVF4PAE4MV4EOEL4ZFTYM7Y45/graph.json","fetch_events":"https://pith.science/api/pith-number/IRVF4PAE4MV4EOEL4ZFTYM7Y45/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IRVF4PAE4MV4EOEL4ZFTYM7Y45/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IRVF4PAE4MV4EOEL4ZFTYM7Y45/action/storage_attestation","attest_author":"https://pith.science/pith/IRVF4PAE4MV4EOEL4ZFTYM7Y45/action/author_attestation","sign_citation":"https://pith.science/pith/IRVF4PAE4MV4EOEL4ZFTYM7Y45/action/citation_signature","submit_replication":"https://pith.science/pith/IRVF4PAE4MV4EOEL4ZFTYM7Y45/action/replication_record"}},"created_at":"2026-07-05T02:31:44.247521+00:00","updated_at":"2026-07-05T02:31:44.247521+00:00"}