{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:MWRO4F23SG4I434X4NBFKYOBLK","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":"92bf61d7acf9cf850910bf88f1d1d4a23991168464ee88d089d5f0176aeffb16","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2017-10-05T12:27:54Z","title_canon_sha256":"8b58e665fd01c0c90270f7f9e96b5d5d33e5f3ca4066123e64789def5b473386"},"schema_version":"1.0","source":{"id":"1710.01981","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.01981","created_at":"2026-05-18T00:33:37Z"},{"alias_kind":"arxiv_version","alias_value":"1710.01981v1","created_at":"2026-05-18T00:33:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.01981","created_at":"2026-05-18T00:33:37Z"},{"alias_kind":"pith_short_12","alias_value":"MWRO4F23SG4I","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_16","alias_value":"MWRO4F23SG4I434X","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_8","alias_value":"MWRO4F23","created_at":"2026-05-18T12:31:31Z"}],"graph_snapshots":[{"event_id":"sha256:e431c28ad196a70a5e04f057eee2f55638fa9481a638eda553fd58cbd7ff2c64","target":"graph","created_at":"2026-05-18T00:33:37Z","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"},"paper":{"abstract_excerpt":"The Mu2e experiment at Fermilab searches for the charged flavor violating conversion of a muon into an electron in the Coulomb field of a nucleus. The detector consists of a straw tube tracker and a CSI crystal electromagnetic calorimeter, both housed in a superconducting solenoid. Both the front-end and the digital electronics, located inside the cryostat, will be operated in vacuum under a 1 T magnetic field, having to sustain the high flux of neutrons and ionizing particles coming from the muons stopping target. These harsh experimental conditions make the design of the calorimeter waveform","authors_text":"E. Pedreschi, F. Spinella, G. Pezzullo, L. Morescalchi, S. Di Falco, S. Donati","cross_cats":["hep-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2017-10-05T12:27:54Z","title":"Components Qualification for a Possible use in the Mu2e Calorimeter Waveform Digitizers"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.01981","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:cea0de2f550df90dadc6a299214b48597f6913217a17f57218d8e329aa27537e","target":"record","created_at":"2026-05-18T00:33:37Z","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":"92bf61d7acf9cf850910bf88f1d1d4a23991168464ee88d089d5f0176aeffb16","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2017-10-05T12:27:54Z","title_canon_sha256":"8b58e665fd01c0c90270f7f9e96b5d5d33e5f3ca4066123e64789def5b473386"},"schema_version":"1.0","source":{"id":"1710.01981","kind":"arxiv","version":1}},"canonical_sha256":"65a2ee175b91b88e6f97e3425561c15a9e8c224d30caf47bd3201b00e6dafc86","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"65a2ee175b91b88e6f97e3425561c15a9e8c224d30caf47bd3201b00e6dafc86","first_computed_at":"2026-05-18T00:33:37.920189Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:33:37.920189Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"td44VXSzBnWsWtyUIp68wq5v81si0SXFrw+NyA1tsmrHGA7L9hIln7NIb239Y8FJlhKgcorRwZ0EXuEH5YQdBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:33:37.920713Z","signed_message":"canonical_sha256_bytes"},"source_id":"1710.01981","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cea0de2f550df90dadc6a299214b48597f6913217a17f57218d8e329aa27537e","sha256:e431c28ad196a70a5e04f057eee2f55638fa9481a638eda553fd58cbd7ff2c64"],"state_sha256":"679ad36de2924efe5e843b17a878e7e87cc3b237d2c0d0b67b21c1c61fa13661"}