{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:BYEX6TAHJUKU33UABGM6BAPFDZ","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":"a56e6c585b7cb85ea228f4f5594cf1d2a42be65fd7d64a9afa68391b030b054b","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-03-31T13:07:52Z","title_canon_sha256":"7875a1ccbbb875e27fd0661abe7aa7c93b5e4eab4c0fdc4ce0e302febbfaf75e"},"schema_version":"1.0","source":{"id":"1603.09572","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1603.09572","created_at":"2026-05-18T01:17:38Z"},{"alias_kind":"arxiv_version","alias_value":"1603.09572v1","created_at":"2026-05-18T01:17:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1603.09572","created_at":"2026-05-18T01:17:38Z"},{"alias_kind":"pith_short_12","alias_value":"BYEX6TAHJUKU","created_at":"2026-05-18T12:30:09Z"},{"alias_kind":"pith_short_16","alias_value":"BYEX6TAHJUKU33UA","created_at":"2026-05-18T12:30:09Z"},{"alias_kind":"pith_short_8","alias_value":"BYEX6TAH","created_at":"2026-05-18T12:30:09Z"}],"graph_snapshots":[{"event_id":"sha256:6bc65a2b0c364088820a75c3e21246d515657fcee3055559866e3a4d6dee985a","target":"graph","created_at":"2026-05-18T01:17:38Z","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 resolution and efficiency of a precision drift-tube chamber for the ATLAS muon spectrometer with final read-out electronics was tested at the Gamma Irradiation Facility at CERN in a 100 GeV muon beam and at photon irradiation rates of up to 990 Hz/square cm which corresponds to twice the highest background rate expected in ATLAS. A silicon strip detector telescope was used as external reference in the beam. The pulse-height measurement of the read-out electronics was used to perform time-slewing corrections which lead to an improvement of the average drift-tube resolution from 104 microns ","authors_text":"A. Manz, A. Staude, F. Rauscher, H. Kroha, J. Dubbert, M. Deile, O. Kortner, R. Richter, S. Horvat, S. Mohrdieck-Moeck, W. Stiller","cross_cats":["hep-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-03-31T13:07:52Z","title":"Resolution and Efficiency of the ATLAS Muon Drift-Tube Chambers at High Background Rates"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1603.09572","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":"sha256:1498f6a236d0a358aee65e167d5319ee938d24dba4ee9cfe95fae46e31a3b813","target":"record","created_at":"2026-05-18T01:17:38Z","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":"a56e6c585b7cb85ea228f4f5594cf1d2a42be65fd7d64a9afa68391b030b054b","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-03-31T13:07:52Z","title_canon_sha256":"7875a1ccbbb875e27fd0661abe7aa7c93b5e4eab4c0fdc4ce0e302febbfaf75e"},"schema_version":"1.0","source":{"id":"1603.09572","kind":"arxiv","version":1}},"canonical_sha256":"0e097f4c074d154dee800999e081e51e710bd3b1bdf359c7395eda3872f543c2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0e097f4c074d154dee800999e081e51e710bd3b1bdf359c7395eda3872f543c2","first_computed_at":"2026-05-18T01:17:38.888305Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:17:38.888305Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"gAmv14mIYlDjJ9Z7FlRoVVuMS/2Ih5kzNOSwnvYUfbGi5y3vKR+B6PVQ9nljpRmW13RjdSop4ond+5UVb5IQDw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:17:38.888985Z","signed_message":"canonical_sha256_bytes"},"source_id":"1603.09572","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1498f6a236d0a358aee65e167d5319ee938d24dba4ee9cfe95fae46e31a3b813","sha256:6bc65a2b0c364088820a75c3e21246d515657fcee3055559866e3a4d6dee985a"],"state_sha256":"709f42dd464cb55aa9d0e2f6790a056459766d9423f23e89d9803e8450dfaa03"}