{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:IKBA3U4FWO7AAJ3SPD3MN2XAVH","short_pith_number":"pith:IKBA3U4F","schema_version":"1.0","canonical_sha256":"42820dd385b3be00277278f6c6eae0a9c9c771f57be028e08948d70e8333c74b","source":{"kind":"arxiv","id":"physics/0610249","version":1},"attestation_state":"computed","paper":{"title":"Contribution of high energy physics techniques to the medical imaging field","license":"","headline":"","cross_cats":[],"primary_cat":"physics.ins-det","authors_text":"B. Joly (LPC-Clermont), G. Montarou (LPC-Clermont), H. Mathez (IPNL), J. Lecoq (LPC-Clermont), M. Boutemeur (IPNL), N. Pauna (LPC-Clermont), P.-E. Vert (LPC-Clermont), P. Le D\\^u (DAPNIA), R. Gaglione (IPNL)","submitted_at":"2006-10-27T06:42:37Z","abstract_excerpt":"The purpose of this study was to show how advanced concepts of compact, lossless and \"Time Of Flight\" (TOF) capable electronics similar to those foreseen for the LHC and ILC experiments could be fairly and easily transferred to the medical imaging field through Positron Emission Tomography (PET). As a wish of explanation, the two overriding weaknesses of PET camera readout electronics, namely dead-time and timing resolution, were investigated analytically and with a Monte-Carlo simulator presently dedicated to this task. Results have shown there was room left for count rate enhancement through"},"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":"physics/0610249","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"physics.ins-det","submitted_at":"2006-10-27T06:42:37Z","cross_cats_sorted":[],"title_canon_sha256":"067fe5a6bd244ed976e714dc3e0d1fcbdf54740b85cae275dc44be9c88d64c82","abstract_canon_sha256":"f7af3c528f0f64e374bc46cdccb0f04641923fbdbe7438cf74e546b2a7fb1a46"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:47:18.661925Z","signature_b64":"O2C2oKgBg+WH58DZjDRPTgywtitm3GeikPHMLo2iDxIuu6OOPX6q/S8WVcaclPYF3A37Vbs5xb/LDD17bst+CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"42820dd385b3be00277278f6c6eae0a9c9c771f57be028e08948d70e8333c74b","last_reissued_at":"2026-07-04T15:47:18.661499Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:47:18.661499Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Contribution of high energy physics techniques to the medical imaging field","license":"","headline":"","cross_cats":[],"primary_cat":"physics.ins-det","authors_text":"B. Joly (LPC-Clermont), G. Montarou (LPC-Clermont), H. Mathez (IPNL), J. Lecoq (LPC-Clermont), M. Boutemeur (IPNL), N. Pauna (LPC-Clermont), P.-E. Vert (LPC-Clermont), P. Le D\\^u (DAPNIA), R. Gaglione (IPNL)","submitted_at":"2006-10-27T06:42:37Z","abstract_excerpt":"The purpose of this study was to show how advanced concepts of compact, lossless and \"Time Of Flight\" (TOF) capable electronics similar to those foreseen for the LHC and ILC experiments could be fairly and easily transferred to the medical imaging field through Positron Emission Tomography (PET). As a wish of explanation, the two overriding weaknesses of PET camera readout electronics, namely dead-time and timing resolution, were investigated analytically and with a Monte-Carlo simulator presently dedicated to this task. Results have shown there was room left for count rate enhancement through"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"physics/0610249","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/physics/0610249/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":"physics/0610249","created_at":"2026-07-04T15:47:18.661565+00:00"},{"alias_kind":"arxiv_version","alias_value":"physics/0610249v1","created_at":"2026-07-04T15:47:18.661565+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.physics/0610249","created_at":"2026-07-04T15:47:18.661565+00:00"},{"alias_kind":"pith_short_12","alias_value":"IKBA3U4FWO7A","created_at":"2026-07-04T15:47:18.661565+00:00"},{"alias_kind":"pith_short_16","alias_value":"IKBA3U4FWO7AAJ3S","created_at":"2026-07-04T15:47:18.661565+00:00"},{"alias_kind":"pith_short_8","alias_value":"IKBA3U4F","created_at":"2026-07-04T15:47:18.661565+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/IKBA3U4FWO7AAJ3SPD3MN2XAVH","json":"https://pith.science/pith/IKBA3U4FWO7AAJ3SPD3MN2XAVH.json","graph_json":"https://pith.science/api/pith-number/IKBA3U4FWO7AAJ3SPD3MN2XAVH/graph.json","events_json":"https://pith.science/api/pith-number/IKBA3U4FWO7AAJ3SPD3MN2XAVH/events.json","paper":"https://pith.science/paper/IKBA3U4F"},"agent_actions":{"view_html":"https://pith.science/pith/IKBA3U4FWO7AAJ3SPD3MN2XAVH","download_json":"https://pith.science/pith/IKBA3U4FWO7AAJ3SPD3MN2XAVH.json","view_paper":"https://pith.science/paper/IKBA3U4F","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=physics/0610249&json=true","fetch_graph":"https://pith.science/api/pith-number/IKBA3U4FWO7AAJ3SPD3MN2XAVH/graph.json","fetch_events":"https://pith.science/api/pith-number/IKBA3U4FWO7AAJ3SPD3MN2XAVH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IKBA3U4FWO7AAJ3SPD3MN2XAVH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IKBA3U4FWO7AAJ3SPD3MN2XAVH/action/storage_attestation","attest_author":"https://pith.science/pith/IKBA3U4FWO7AAJ3SPD3MN2XAVH/action/author_attestation","sign_citation":"https://pith.science/pith/IKBA3U4FWO7AAJ3SPD3MN2XAVH/action/citation_signature","submit_replication":"https://pith.science/pith/IKBA3U4FWO7AAJ3SPD3MN2XAVH/action/replication_record"}},"created_at":"2026-07-04T15:47:18.661565+00:00","updated_at":"2026-07-04T15:47:18.661565+00:00"}