{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:CD7MHUYNNT2JL3AZI3CCKJJAMY","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":"19df8757c7108399403ed778f99fd662823f3a11cddaf16f42e8545f257a8ca4","cross_cats_sorted":["astro-ph.IM","hep-ex","nucl-ex"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2023-11-09T12:40:48Z","title_canon_sha256":"aaf505e220389db63dca87a6dcc02f6ef72b1b05ae826a82c483174369ce60a3"},"schema_version":"1.0","source":{"id":"2311.05320","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2311.05320","created_at":"2026-07-05T07:40:42Z"},{"alias_kind":"arxiv_version","alias_value":"2311.05320v2","created_at":"2026-07-05T07:40:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.05320","created_at":"2026-07-05T07:40:42Z"},{"alias_kind":"pith_short_12","alias_value":"CD7MHUYNNT2J","created_at":"2026-07-05T07:40:42Z"},{"alias_kind":"pith_short_16","alias_value":"CD7MHUYNNT2JL3AZ","created_at":"2026-07-05T07:40:42Z"},{"alias_kind":"pith_short_8","alias_value":"CD7MHUYN","created_at":"2026-07-05T07:40:42Z"}],"graph_snapshots":[{"event_id":"sha256:5bde0499c4d03f23ce84a396f130fff1a9be38eaab37bbd0f2d0664e6f9d87dd","target":"graph","created_at":"2026-07-05T07:40:42Z","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/2311.05320/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In the past decade, dual-phase xenon time projection chambers (Xe-TPCs) have emerged as some of the most powerful detectors in the fields of astroparticle physics and rare-event searches. Developed primarily towards the direct detection of dark matter particles, experiments presently operating deep underground have reached target masses at the multi-tonne scale, energy thresholds around 1 keV and radioactivity-induced background rates similar to those from solar neutrinos. These unique properties, together with demonstrated stable operation over several years, allow for the exploration of new ","authors_text":"Laura Baudis","cross_cats":["astro-ph.IM","hep-ex","nucl-ex"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2023-11-09T12:40:48Z","title":"Dual-phase xenon time projection chambers for rare-event searches"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.05320","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":"sha256:555a422c05d1bf611cef70dd23df13e631ccd3e2f7e4ff47cf3d710fb858491a","target":"record","created_at":"2026-07-05T07:40:42Z","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":"19df8757c7108399403ed778f99fd662823f3a11cddaf16f42e8545f257a8ca4","cross_cats_sorted":["astro-ph.IM","hep-ex","nucl-ex"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2023-11-09T12:40:48Z","title_canon_sha256":"aaf505e220389db63dca87a6dcc02f6ef72b1b05ae826a82c483174369ce60a3"},"schema_version":"1.0","source":{"id":"2311.05320","kind":"arxiv","version":2}},"canonical_sha256":"10fec3d30d6cf495ec1946c42525206613f3bea2517e34d3a7182c97d9d6045c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"10fec3d30d6cf495ec1946c42525206613f3bea2517e34d3a7182c97d9d6045c","first_computed_at":"2026-07-05T07:40:42.989103Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T07:40:42.989103Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"I1TIwDuRAr2pYwGEGMqWpq4SV6pPzk5dwTRdFkKozTdXEuGaEX7vkqYHJ3KVB/sTW7qX2UWRZpCbAgnRJPXvBA==","signature_status":"signed_v1","signed_at":"2026-07-05T07:40:42.989568Z","signed_message":"canonical_sha256_bytes"},"source_id":"2311.05320","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:555a422c05d1bf611cef70dd23df13e631ccd3e2f7e4ff47cf3d710fb858491a","sha256:5bde0499c4d03f23ce84a396f130fff1a9be38eaab37bbd0f2d0664e6f9d87dd"],"state_sha256":"ae76b3863035bfb9e29be82c28ad191a3bbff617e30e2d87983571b2322f1463"}