{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:FJJXYUD2OG5X5LYJQ3AYTGMWB4","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":"e487eafd045b8c05f37e5264457d23adb82b430737a8b65621e16666213e7924","cross_cats_sorted":["nucl-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-02-24T05:31:44Z","title_canon_sha256":"dda7570d1e96ed53360d098c178ba103d3749c3668c02e14ea12a6ddd0946d18"},"schema_version":"1.0","source":{"id":"1602.07401","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1602.07401","created_at":"2026-05-18T01:03:30Z"},{"alias_kind":"arxiv_version","alias_value":"1602.07401v1","created_at":"2026-05-18T01:03:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.07401","created_at":"2026-05-18T01:03:30Z"},{"alias_kind":"pith_short_12","alias_value":"FJJXYUD2OG5X","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_16","alias_value":"FJJXYUD2OG5X5LYJ","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_8","alias_value":"FJJXYUD2","created_at":"2026-05-18T12:30:15Z"}],"graph_snapshots":[{"event_id":"sha256:580c153419c735e48512426ed065aced183abfe88677d867c2bd3c0edac357ee","target":"graph","created_at":"2026-05-18T01:03:30Z","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":"We report the development of a CaMoO4 crystal low temperature detector for the AMoRE neutrinoless double beta decay (0{\\nu}\\b{eta}\\b{eta}) search experiment. The prototype detector cell was composed of a 216 g CaMoO4 crystal and a metallic magnetic calorimeter. An over-ground measurement demonstrated FWHM resolution of 6-11 keV for full absorption gamma peaks. Pulse shape discrimination was clearly demonstrated in the phonon signals, and 7.6 {\\sigma} of discrimination power was found for the {\\alpha} and \\b{eta}/{\\gamma} separation. The phonon signals showed rise-times of about 1 ms. It is exp","authors_text":"A. Fleischmann, C.S. Kang, F.A. Danevich, G.B. Kim, H.J. Kim, H.J. Lee, J.H. Lee, J.H. So, M.K. Lee, S. Choi, S.J. Lee, S.R. Kim, V.A. Kornoukhov, W.S. Yoon, Y.D. Kim, Y.H. Kim","cross_cats":["nucl-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-02-24T05:31:44Z","title":"A CaMoO4 Crystal Low Temperature Detector for the AMoRE Neutrinoless Double Beta Decay Search"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.07401","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":"sha256:86a99a73e834dbaf4216dce8b2482b9052b7ef2b9b9f677019a7666b76989706","target":"record","created_at":"2026-05-18T01:03:30Z","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":"e487eafd045b8c05f37e5264457d23adb82b430737a8b65621e16666213e7924","cross_cats_sorted":["nucl-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-02-24T05:31:44Z","title_canon_sha256":"dda7570d1e96ed53360d098c178ba103d3749c3668c02e14ea12a6ddd0946d18"},"schema_version":"1.0","source":{"id":"1602.07401","kind":"arxiv","version":1}},"canonical_sha256":"2a537c507a71bb7eaf0986c18999960f287b6b213ced190d21a48f749546dcba","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2a537c507a71bb7eaf0986c18999960f287b6b213ced190d21a48f749546dcba","first_computed_at":"2026-05-18T01:03:30.683237Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:03:30.683237Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"6558MMwPyz5Tpvpr/U71VSdvE9+Hn6M5blsSZwOtqmdv7VoqbXm1Kn/y/SbfD0ZwYQU+Vlg6rq/u2vIQdI75Bw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:03:30.683757Z","signed_message":"canonical_sha256_bytes"},"source_id":"1602.07401","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:86a99a73e834dbaf4216dce8b2482b9052b7ef2b9b9f677019a7666b76989706","sha256:580c153419c735e48512426ed065aced183abfe88677d867c2bd3c0edac357ee"],"state_sha256":"61e2caef1fde8c0564b097ae74634e1a8f45128446c25783d1c1949e9a24b990"}