{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2020:GPKVIMKZEAIAQVDOBEXATAQBTP","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":"427eddc2ab3e91b6a103866c5328e4a51f7780cd40f4885d396d0bce86651205","cross_cats_sorted":["physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.IM","submitted_at":"2020-12-15T10:07:19Z","title_canon_sha256":"51c9c423f6fdd331d7298a7b4062d04a42659348ddfdf9185f88b93e99eadfa8"},"schema_version":"1.0","source":{"id":"2012.08186","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2012.08186","created_at":"2026-07-05T01:59:41Z"},{"alias_kind":"arxiv_version","alias_value":"2012.08186v1","created_at":"2026-07-05T01:59:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2012.08186","created_at":"2026-07-05T01:59:41Z"},{"alias_kind":"pith_short_12","alias_value":"GPKVIMKZEAIA","created_at":"2026-07-05T01:59:41Z"},{"alias_kind":"pith_short_16","alias_value":"GPKVIMKZEAIAQVDO","created_at":"2026-07-05T01:59:41Z"},{"alias_kind":"pith_short_8","alias_value":"GPKVIMKZ","created_at":"2026-07-05T01:59:41Z"}],"graph_snapshots":[{"event_id":"sha256:282071c157552411aa220b800591e0705a8309d903622fd99264320f22033d95","target":"graph","created_at":"2026-07-05T01:59:41Z","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/2012.08186/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The Teledyne HxRG detectors have versatile and programmable output options to allow operation of them in a variety of configurations such as slow unbuffered, slow buffered, fast buffered or unbuffered modes to optimise the detector performance for a given application. Normally at ESO, for low noise operation, the detectors are operated in slow unbuffered mode. Whilst the slow unbuffered mode offers a simple interface to the external preamplifier electronics, the detector operation in this mode can suffer from reduced pixel frequency response and higher electrical crosstalk between the readout ","authors_text":"Beno\\^it Serra, Christopher Mandla, Derek Ives, Domingo Alvarez, Elizabeth George, Leander Mehrgan, Naidu Bezawada","cross_cats":["physics.ins-det"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.IM","submitted_at":"2020-12-15T10:07:19Z","title":"Performance advantages of buffered mode operation of HxRG near infrared detectors"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2012.08186","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:ec287e56885aa8de075b92176f5c98ca16ce34fc692ec6aa50792fad818a084b","target":"record","created_at":"2026-07-05T01:59:41Z","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":"427eddc2ab3e91b6a103866c5328e4a51f7780cd40f4885d396d0bce86651205","cross_cats_sorted":["physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.IM","submitted_at":"2020-12-15T10:07:19Z","title_canon_sha256":"51c9c423f6fdd331d7298a7b4062d04a42659348ddfdf9185f88b93e99eadfa8"},"schema_version":"1.0","source":{"id":"2012.08186","kind":"arxiv","version":1}},"canonical_sha256":"33d5543159201008546e092e0982019be8061e1b7dc80c6464b16df1e27ac539","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"33d5543159201008546e092e0982019be8061e1b7dc80c6464b16df1e27ac539","first_computed_at":"2026-07-05T01:59:41.066985Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T01:59:41.066985Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"CbmlCy29p+KTQVO0f+yzbjGOy5+ahPnM3Ykfwzo1mLzFB9RllqrsRoOVAj+1VwZepynQTmyKEteyHbOt+cC4Bg==","signature_status":"signed_v1","signed_at":"2026-07-05T01:59:41.067402Z","signed_message":"canonical_sha256_bytes"},"source_id":"2012.08186","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ec287e56885aa8de075b92176f5c98ca16ce34fc692ec6aa50792fad818a084b","sha256:282071c157552411aa220b800591e0705a8309d903622fd99264320f22033d95"],"state_sha256":"13c1241eb35c2718b7360780fa88e4da28e22ced22955ce1708aed7fae270030"}