{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:2CB5IGJPHAA46A3M534SSRIVHV","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":"2359536530402131f7d41f57f11e7d16bf14417f63111e7ffd977be676b3485c","cross_cats_sorted":["physics.ins-det"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2024-01-08T18:25:40Z","title_canon_sha256":"09563894a961f7619ed62c77a44077458ca71d0e21e1b8d06f2a282873149972"},"schema_version":"1.0","source":{"id":"2401.04074","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2401.04074","created_at":"2026-07-05T07:31:37Z"},{"alias_kind":"arxiv_version","alias_value":"2401.04074v2","created_at":"2026-07-05T07:31:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2401.04074","created_at":"2026-07-05T07:31:37Z"},{"alias_kind":"pith_short_12","alias_value":"2CB5IGJPHAA4","created_at":"2026-07-05T07:31:37Z"},{"alias_kind":"pith_short_16","alias_value":"2CB5IGJPHAA46A3M","created_at":"2026-07-05T07:31:37Z"},{"alias_kind":"pith_short_8","alias_value":"2CB5IGJP","created_at":"2026-07-05T07:31:37Z"}],"graph_snapshots":[{"event_id":"sha256:ae6d07a6d3d8281a920cd8d4d6d5b51d1a1fbbd7ebaf87283c9ab7dafae55317","target":"graph","created_at":"2026-07-05T07:31:37Z","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/2401.04074/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The recent detection of coherent elastic neutrino-nucleus scattering (CE$\\nu$NS) opens the possibility to use neutrinos to explore physics beyond standard model, with small-size detectors. However, the CE$\\nu$NS process generates signals at the few keV level, requiring very sensitive detector technologies. The European Spallation Source (ESS) has been identified as an optimal source of low energy neutrinos, offering an opportunity for a definitive exploration of all phenomenological applications of CE$\\nu$NS. A number of different detector approaches are currently under development for deploym","authors_text":"A. Sim\\'on (on behalf of the $\\nu$ESS collaboration)","cross_cats":["physics.ins-det"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2024-01-08T18:25:40Z","title":"CE$\\nu$NS at the European Spallation Source"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2401.04074","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":"sha256:35d24af0530d369c36a7a9043385136fb12c34416545913867eed09f5ea69400","target":"record","created_at":"2026-07-05T07:31:37Z","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":"2359536530402131f7d41f57f11e7d16bf14417f63111e7ffd977be676b3485c","cross_cats_sorted":["physics.ins-det"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2024-01-08T18:25:40Z","title_canon_sha256":"09563894a961f7619ed62c77a44077458ca71d0e21e1b8d06f2a282873149972"},"schema_version":"1.0","source":{"id":"2401.04074","kind":"arxiv","version":2}},"canonical_sha256":"d083d4192f3801cf036ceef92945153d4f59ad6638d89e2d110288a65d573659","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d083d4192f3801cf036ceef92945153d4f59ad6638d89e2d110288a65d573659","first_computed_at":"2026-07-05T07:31:37.319590Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T07:31:37.319590Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"NMH/puuh8bXr0bOUUOk8KOroSDCkg/bdDbTUB8xscgaVf1B71WX1scmBDqXg2Qk3GrvTLZoY5u+5261I3xsmAg==","signature_status":"signed_v1","signed_at":"2026-07-05T07:31:37.320046Z","signed_message":"canonical_sha256_bytes"},"source_id":"2401.04074","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:35d24af0530d369c36a7a9043385136fb12c34416545913867eed09f5ea69400","sha256:ae6d07a6d3d8281a920cd8d4d6d5b51d1a1fbbd7ebaf87283c9ab7dafae55317"],"state_sha256":"c7742a90d735fff12702bbc81f554525ad5f3e00f7229f460fe57c6fe1698b44"}