{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:5WUJVATVBJBQHS5I3XIZRJYUS5","short_pith_number":"pith:5WUJVATV","canonical_record":{"source":{"id":"1607.07694","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-07-26T13:50:49Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"842da5604ca701aa91419c9d6c3e4567d962be9357e1ea3dd669fe76de1386b1","abstract_canon_sha256":"8acd2f669bb166b05118eed6beca5f4e5d85f288bb817835c93ce72d69243dec"},"schema_version":"1.0"},"canonical_sha256":"eda89a82750a4303cba8ddd198a714975fb394ff69dfb66a5d3be0ce4cff17bf","source":{"kind":"arxiv","id":"1607.07694","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1607.07694","created_at":"2026-05-18T01:00:52Z"},{"alias_kind":"arxiv_version","alias_value":"1607.07694v2","created_at":"2026-05-18T01:00:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.07694","created_at":"2026-05-18T01:00:52Z"},{"alias_kind":"pith_short_12","alias_value":"5WUJVATVBJBQ","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_16","alias_value":"5WUJVATVBJBQHS5I","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_8","alias_value":"5WUJVATV","created_at":"2026-05-18T12:30:01Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:5WUJVATVBJBQHS5I3XIZRJYUS5","target":"record","payload":{"canonical_record":{"source":{"id":"1607.07694","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-07-26T13:50:49Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"842da5604ca701aa91419c9d6c3e4567d962be9357e1ea3dd669fe76de1386b1","abstract_canon_sha256":"8acd2f669bb166b05118eed6beca5f4e5d85f288bb817835c93ce72d69243dec"},"schema_version":"1.0"},"canonical_sha256":"eda89a82750a4303cba8ddd198a714975fb394ff69dfb66a5d3be0ce4cff17bf","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:00:52.653528Z","signature_b64":"Lq8PEICbE6u3EeVr0AWFDXLqQHT7LNYUZV0EaY1PnaR8aAeOvjpKZviefzAA0pRtYf4lW6Kr/U/g8Bm+XNoPAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"eda89a82750a4303cba8ddd198a714975fb394ff69dfb66a5d3be0ce4cff17bf","last_reissued_at":"2026-05-18T01:00:52.652907Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:00:52.652907Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1607.07694","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:00:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vEU+JUcieD8RrecELAoe8mYLjiyEp2BYFnpfDqp0NgCvkPAK3gjkzvijatoQ13KCxMHhib11mQO8pymPH8B7Aw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T23:02:22.068477Z"},"content_sha256":"41bf04a45fd994f04dfa64bfbaabf1f9bd90159fd3c1b5655fc9f6ca95a125d4","schema_version":"1.0","event_id":"sha256:41bf04a45fd994f04dfa64bfbaabf1f9bd90159fd3c1b5655fc9f6ca95a125d4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:5WUJVATVBJBQHS5I3XIZRJYUS5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"On drift fields in CMOS Monolithic Active Pixel Sensors with point-like collection diodes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"physics.ins-det","authors_text":"A. Dorokhov, B. Linnik, C. M\\\"untz, D. Doering, J. Baudot, J. Heymes, J. Stroth, M. Deveaux, M. Kachel, M. Koziel","submitted_at":"2016-07-26T13:50:49Z","abstract_excerpt":"- Paper withdrawn by the author - CMOS Monolithic Active Pixel Sensors for charged particle tracking are considered as technology for numerous experiments in heavy ion and particle physics. To match the requirements for those applications in terms of tolerance to non-ionizing radiation, it is being tried to deplete the sensitive volume of the, traditionally non-depleted, silicon sensors.\n  We study the feasibility of this approach for the common case that the collection diodes of the pixel are small as compared to the pixel pitch. An analytic equation predicting the thickness of the depletion "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.07694","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:00:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0/dkxyxLGYvkfXrP4/vG/ML37f+pOweKphVT/UBckHL4yWDyecj+H7XcukCOzFR7Cp1Tr9emovlv/afImy/uCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T23:02:22.068820Z"},"content_sha256":"acea81686f91adfe2685b6b13719e0813e36607a388c92b2990421f82738df01","schema_version":"1.0","event_id":"sha256:acea81686f91adfe2685b6b13719e0813e36607a388c92b2990421f82738df01"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5WUJVATVBJBQHS5I3XIZRJYUS5/bundle.json","state_url":"https://pith.science/pith/5WUJVATVBJBQHS5I3XIZRJYUS5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5WUJVATVBJBQHS5I3XIZRJYUS5/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-01T23:02:22Z","links":{"resolver":"https://pith.science/pith/5WUJVATVBJBQHS5I3XIZRJYUS5","bundle":"https://pith.science/pith/5WUJVATVBJBQHS5I3XIZRJYUS5/bundle.json","state":"https://pith.science/pith/5WUJVATVBJBQHS5I3XIZRJYUS5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5WUJVATVBJBQHS5I3XIZRJYUS5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:5WUJVATVBJBQHS5I3XIZRJYUS5","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"8acd2f669bb166b05118eed6beca5f4e5d85f288bb817835c93ce72d69243dec","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-07-26T13:50:49Z","title_canon_sha256":"842da5604ca701aa91419c9d6c3e4567d962be9357e1ea3dd669fe76de1386b1"},"schema_version":"1.0","source":{"id":"1607.07694","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1607.07694","created_at":"2026-05-18T01:00:52Z"},{"alias_kind":"arxiv_version","alias_value":"1607.07694v2","created_at":"2026-05-18T01:00:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.07694","created_at":"2026-05-18T01:00:52Z"},{"alias_kind":"pith_short_12","alias_value":"5WUJVATVBJBQ","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_16","alias_value":"5WUJVATVBJBQHS5I","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_8","alias_value":"5WUJVATV","created_at":"2026-05-18T12:30:01Z"}],"graph_snapshots":[{"event_id":"sha256:acea81686f91adfe2685b6b13719e0813e36607a388c92b2990421f82738df01","target":"graph","created_at":"2026-05-18T01:00:52Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"- Paper withdrawn by the author - CMOS Monolithic Active Pixel Sensors for charged particle tracking are considered as technology for numerous experiments in heavy ion and particle physics. To match the requirements for those applications in terms of tolerance to non-ionizing radiation, it is being tried to deplete the sensitive volume of the, traditionally non-depleted, silicon sensors.\n  We study the feasibility of this approach for the common case that the collection diodes of the pixel are small as compared to the pixel pitch. An analytic equation predicting the thickness of the depletion ","authors_text":"A. Dorokhov, B. Linnik, C. M\\\"untz, D. Doering, J. Baudot, J. Heymes, J. Stroth, M. Deveaux, M. Kachel, M. Koziel","cross_cats":["hep-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-07-26T13:50:49Z","title":"On drift fields in CMOS Monolithic Active Pixel Sensors with point-like collection diodes"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.07694","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:41bf04a45fd994f04dfa64bfbaabf1f9bd90159fd3c1b5655fc9f6ca95a125d4","target":"record","created_at":"2026-05-18T01:00:52Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"8acd2f669bb166b05118eed6beca5f4e5d85f288bb817835c93ce72d69243dec","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-07-26T13:50:49Z","title_canon_sha256":"842da5604ca701aa91419c9d6c3e4567d962be9357e1ea3dd669fe76de1386b1"},"schema_version":"1.0","source":{"id":"1607.07694","kind":"arxiv","version":2}},"canonical_sha256":"eda89a82750a4303cba8ddd198a714975fb394ff69dfb66a5d3be0ce4cff17bf","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"eda89a82750a4303cba8ddd198a714975fb394ff69dfb66a5d3be0ce4cff17bf","first_computed_at":"2026-05-18T01:00:52.652907Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:00:52.652907Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Lq8PEICbE6u3EeVr0AWFDXLqQHT7LNYUZV0EaY1PnaR8aAeOvjpKZviefzAA0pRtYf4lW6Kr/U/g8Bm+XNoPAg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:00:52.653528Z","signed_message":"canonical_sha256_bytes"},"source_id":"1607.07694","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:41bf04a45fd994f04dfa64bfbaabf1f9bd90159fd3c1b5655fc9f6ca95a125d4","sha256:acea81686f91adfe2685b6b13719e0813e36607a388c92b2990421f82738df01"],"state_sha256":"13b5c777b6ef152ca05d90b8f646bda2d6f910fb0131980c3865f7af3ca220b6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ljRIuimgIDRFia77UfjyRcxA7d1eTP3lmOpNKdPIpaQJGVoSK4DTNrGOFRHibBKQus6dIxec16ux/lONJXW2AQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T23:02:22.070754Z","bundle_sha256":"4991cd7c4ecd76091c3dc9b1ba6b8d6dc921e9ad6b93ad9a0e45fa06f6e7ef02"}}