{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:6NWWP6FMDSK6CTEIPAXA7C4FTU","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":"b1e55fe3108b30b7d0b161de634a6ea87ff65c4588d75f6f8a2f08d1c85b5d46","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2022-10-26T13:19:24Z","title_canon_sha256":"6ad1a22154c809fce098d420f7cb0911d72a83520c163010002472ff3faa994d"},"schema_version":"1.0","source":{"id":"2210.14690","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2210.14690","created_at":"2026-07-05T05:59:04Z"},{"alias_kind":"arxiv_version","alias_value":"2210.14690v1","created_at":"2026-07-05T05:59:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2210.14690","created_at":"2026-07-05T05:59:04Z"},{"alias_kind":"pith_short_12","alias_value":"6NWWP6FMDSK6","created_at":"2026-07-05T05:59:04Z"},{"alias_kind":"pith_short_16","alias_value":"6NWWP6FMDSK6CTEI","created_at":"2026-07-05T05:59:04Z"},{"alias_kind":"pith_short_8","alias_value":"6NWWP6FM","created_at":"2026-07-05T05:59:04Z"}],"graph_snapshots":[{"event_id":"sha256:2a6df900c00441a158675089de38ca443dbb86c67c3ba996be406bdc5476fca8","target":"graph","created_at":"2026-07-05T05:59:04Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2210.14690/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Single-crystal synthetic diamond sensors have been widely used in radiation dosimetry and beam diagnostics. The foreseen harsh radiation environment in electron-positron colliders at the luminosity frontier requires a thorough investigation of diamond's response to large radiation burst, in particular, to intense high-energy electron pulses. In this article, a two-step numerical simulation approach (Sentaurus~+~LTspice) is proposed to explore this topic. Time response of the diamond detector is simulated via TCAD-Sentaurus while the transmission effect of the electronic circuit is taken into a","authors_text":"A. Gabrielli, P. Cristaudo, Y. Jin","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2022-10-26T13:19:24Z","title":"Simulation of the response of a diamond-based radiation detector to ultra-short and intense high-energy electron pulses"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2210.14690","kind":"arxiv","version":1},"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":"sha256:549078c72a81c61fd4d4617f921d286a0eb29e8eb8463e4457380039413a507d","target":"record","created_at":"2026-07-05T05:59:04Z","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":"b1e55fe3108b30b7d0b161de634a6ea87ff65c4588d75f6f8a2f08d1c85b5d46","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2022-10-26T13:19:24Z","title_canon_sha256":"6ad1a22154c809fce098d420f7cb0911d72a83520c163010002472ff3faa994d"},"schema_version":"1.0","source":{"id":"2210.14690","kind":"arxiv","version":1}},"canonical_sha256":"f36d67f8ac1c95e14c88782e0f8b859d01a540d62c0baf7436069c886f3eeb68","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f36d67f8ac1c95e14c88782e0f8b859d01a540d62c0baf7436069c886f3eeb68","first_computed_at":"2026-07-05T05:59:04.794171Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:59:04.794171Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"1OWpyXksilO2nod8kTkeRbuivSgShhOqdlRhdCKf0xtdYZpE62rcaBGNqNu7xF1PTz97tRzwmkyCTAF6jq8ADw==","signature_status":"signed_v1","signed_at":"2026-07-05T05:59:04.794718Z","signed_message":"canonical_sha256_bytes"},"source_id":"2210.14690","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:549078c72a81c61fd4d4617f921d286a0eb29e8eb8463e4457380039413a507d","sha256:2a6df900c00441a158675089de38ca443dbb86c67c3ba996be406bdc5476fca8"],"state_sha256":"03a85975924e2e7d97a287f9281cbba9840693b8cf096b5400aea691e82bbc80"}