{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:SKJO77OYAB4KK2FXQSYU5B4VCC","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":"f8143c3ece51db517f9c2ae020ec049a6a489d0ca1eb8cbedff14792e61663f1","cross_cats_sorted":["nucl-ex"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2026-07-29T10:22:47Z","title_canon_sha256":"7939f678e99a68431a41d28e1cc874a27c4a77f8c44303a7eb42d70837ed0811"},"schema_version":"1.0","source":{"id":"2607.26732","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2607.26732","created_at":"2026-07-30T01:22:07Z"},{"alias_kind":"arxiv_version","alias_value":"2607.26732v1","created_at":"2026-07-30T01:22:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.26732","created_at":"2026-07-30T01:22:07Z"},{"alias_kind":"pith_short_12","alias_value":"SKJO77OYAB4K","created_at":"2026-07-30T01:22:07Z"},{"alias_kind":"pith_short_16","alias_value":"SKJO77OYAB4KK2FX","created_at":"2026-07-30T01:22:07Z"},{"alias_kind":"pith_short_8","alias_value":"SKJO77OY","created_at":"2026-07-30T01:22:07Z"}],"graph_snapshots":[{"event_id":"sha256:60df0753c06e541ac2296ef4e7593d6d19e7e7e08df81cac6e347a191ab381be","target":"graph","created_at":"2026-07-30T01:22:07Z","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/2607.26732/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The CROSS experiment to search for neutrinoless double-beta ($0\\nu2\\beta$) decay in $^{100}$Mo with the help of an array of scintillating cryogenic calorimeters, containing 4.9 kg of $^{100}$Mo, has been ongoing in a low-background setup at the Canfranc underground laboratory (Spain) since mid-November 2025. In this paper, we present the construction of the CROSS detector and the description of Geant4-based Monte Carlo simulations of expected background in the region of interest. The simulations predict the background index in a 100-keV-wide interval centered at the $Q$-value of $^{100}$Mo (30","authors_text":"A. Drobizhev, A. Giuliani, A. Ianni, A. Ortiz de Sol\\'orzano, A.S. Barabash, A. Zolotarova, B. Schmidt, C.A. Marrache-Kikuchi, C. Gotti, C. Nones, D. Auguste, D. Cintas, D.V. Poda, E. Olivieri, F.A. Danevich, F. Ferri, G. Benato, G. Pessina, I. Cojocari, I. Dafinei, J. Cao, J.M. Calvo-Mozota, L. Berg\\'e, L. Dumoulin, M. Buchynska, M. Chapellier, M. De Deo, M. Martinez, M. Pageot, M. Velazquez, M. Zarytskyy, P. Carniti, P. de Marcillac, Ph. Gras, Ph. Rosier, P. Loaiza, R. Serino, S.I. Konovalov, S. Marnieros, V. Berest, V.I. Tretyak, V.I. Umatov, V.V. Kobychev, Y. Peinaud, Yu. G. Kolomensky","cross_cats":["nucl-ex"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2026-07-29T10:22:47Z","title":"The CROSS experiment: detector construction, background projection, and sensitivity to $^{100}$Mo $0\\nu2\\beta$ decay"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.26732","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":"sha256:02675e239f20300d337f72c92b56b1603a71e6c53a96e915873ba81c37dcf819","target":"record","created_at":"2026-07-30T01:22:07Z","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":"f8143c3ece51db517f9c2ae020ec049a6a489d0ca1eb8cbedff14792e61663f1","cross_cats_sorted":["nucl-ex"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2026-07-29T10:22:47Z","title_canon_sha256":"7939f678e99a68431a41d28e1cc874a27c4a77f8c44303a7eb42d70837ed0811"},"schema_version":"1.0","source":{"id":"2607.26732","kind":"arxiv","version":1}},"canonical_sha256":"9292effdd80078a568b784b14e879510a41a779c11374572b9d44b52ae12df88","receipt":{"builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9292effdd80078a568b784b14e879510a41a779c11374572b9d44b52ae12df88","first_computed_at":"2026-07-30T01:22:07.855469Z","kind":"pith_receipt","last_reissued_at":"2026-07-30T01:22:07.855469Z","receipt_version":"0.3","signature_status":"unsigned_v0"},"source_id":"2607.26732","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:02675e239f20300d337f72c92b56b1603a71e6c53a96e915873ba81c37dcf819","sha256:60df0753c06e541ac2296ef4e7593d6d19e7e7e08df81cac6e347a191ab381be"],"state_sha256":"2ebffe092dffbf3fcf47e1cbfff5adb513b5cc968ebce4165096378176ab2249"}