{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:6OENTBDKHPJAOIQP7HCYBHTFEY","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":"306f52a1dd1b8104bedf716a95f5345f111d91bbfa53687a635ee11c2576143e","cross_cats_sorted":["physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2019-11-06T15:47:13Z","title_canon_sha256":"cd93e7e05664521e227780efeb0a75868bcdbdb4a53835704aaa5ed98c772381"},"schema_version":"1.0","source":{"id":"1911.02446","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1911.02446","created_at":"2026-07-05T00:17:34Z"},{"alias_kind":"arxiv_version","alias_value":"1911.02446v1","created_at":"2026-07-05T00:17:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1911.02446","created_at":"2026-07-05T00:17:34Z"},{"alias_kind":"pith_short_12","alias_value":"6OENTBDKHPJA","created_at":"2026-07-05T00:17:34Z"},{"alias_kind":"pith_short_16","alias_value":"6OENTBDKHPJAOIQP","created_at":"2026-07-05T00:17:34Z"},{"alias_kind":"pith_short_8","alias_value":"6OENTBDK","created_at":"2026-07-05T00:17:34Z"}],"graph_snapshots":[{"event_id":"sha256:872c91be38041df43cd8454fffef6b77b58a05619a643f587e6e92c5aa9d222b","target":"graph","created_at":"2026-07-05T00:17:34Z","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/1911.02446/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present the search for Lorentz violation in the double beta decay of ^{82}Se~with CUPID-0, using an exposure of 9.95 kg x y. We found no evidence for the searched signal and set a limit on the isotropic components of the Lorentz violating coefficient of $\\mathring{a}_{\\text{of}}^{(3)} < 4.1\\cdot10^{-6}$ GeV (90\\% Credible Interval). This results is obtained with a Bayesian analysis of the experimental data and fully includes the systematic uncertainties of the model. This is the first limit on $\\mathring{a}_{\\text{of}}^{(3)}$ obtained with a scintillating bolometer, showing the potentiality","authors_text":"A. Cruciani, A. Giuliani, A. Puiu, A. Zolotarova, C. Brofferio, C. Bucci, C. Gotti, C. Nones, C. Rusconi, C. Tomei, D. Chiesa, D. Orlandi, E. Previtali, F. Bellini, F. Ferroni, G. Keppel, G. Pessina, I. Dafinei, I. Nutini, J.W. Beeman, K. Schaffner, L. Cardani, L. Gironi, L. Pagnanini, L. Pattavina, M. Beretta, M. Biassoni, M. Clemenza, M. Martinez, M. Nastasi, M. Pallavicini, M. Pavan, M. Vignati, N. Casali, O. Azzolini, O. Cremonesi, P. Carniti, P. Gorla, S. Capelli, S. Di Domizio, S. Nagorny, S. Nisi, S. Pirro, S. Pozzi, V. Pettinacci","cross_cats":["physics.ins-det"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2019-11-06T15:47:13Z","title":"First search for Lorentz violation in double beta decay with scintillating calorimeters"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1911.02446","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":"sha256:546d382a17314cd96189cc988d8045e802defe4c2df5439dec26d4bc0bc57026","target":"record","created_at":"2026-07-05T00:17:34Z","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":"306f52a1dd1b8104bedf716a95f5345f111d91bbfa53687a635ee11c2576143e","cross_cats_sorted":["physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2019-11-06T15:47:13Z","title_canon_sha256":"cd93e7e05664521e227780efeb0a75868bcdbdb4a53835704aaa5ed98c772381"},"schema_version":"1.0","source":{"id":"1911.02446","kind":"arxiv","version":1}},"canonical_sha256":"f388d9846a3bd207220ff9c5809e65260936acda6c071e558abf3e90bedaefb5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f388d9846a3bd207220ff9c5809e65260936acda6c071e558abf3e90bedaefb5","first_computed_at":"2026-07-05T00:17:34.417775Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T00:17:34.417775Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"7+ka8F2jNAT7xj3S9Z2sbM3rwOlYuuwOAfp5TJY/2o1ebGliaz8NBaO14/ZPpb1axamGPEtPtqXLfM1y6tT9CA==","signature_status":"signed_v1","signed_at":"2026-07-05T00:17:34.418263Z","signed_message":"canonical_sha256_bytes"},"source_id":"1911.02446","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:546d382a17314cd96189cc988d8045e802defe4c2df5439dec26d4bc0bc57026","sha256:872c91be38041df43cd8454fffef6b77b58a05619a643f587e6e92c5aa9d222b"],"state_sha256":"b5274fd0a6c84ea2c9d008fd3444cb5ac35e6c74bd9eabe024bfa6af9eadebaa"}