{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:7G4XBQBP5P2YIBUJRP4AWXBPL5","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":"727b4982e559dadb4508bde20959da7bb72244db3f962b91b7438e895aa4b0b6","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-05-09T12:37:19Z","title_canon_sha256":"b237c1dbb6f7d1329684e36c3c1e20d80950256f0bdf18abc26e0403f7055282"},"schema_version":"1.0","source":{"id":"1605.02558","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1605.02558","created_at":"2026-05-18T01:02:44Z"},{"alias_kind":"arxiv_version","alias_value":"1605.02558v1","created_at":"2026-05-18T01:02:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.02558","created_at":"2026-05-18T01:02:44Z"},{"alias_kind":"pith_short_12","alias_value":"7G4XBQBP5P2Y","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_16","alias_value":"7G4XBQBP5P2YIBUJ","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_8","alias_value":"7G4XBQBP","created_at":"2026-05-18T12:30:04Z"}],"graph_snapshots":[{"event_id":"sha256:55a350b26d05dea57b7184e550037858e65f995691b0fce2423e21fad7d516ac","target":"graph","created_at":"2026-05-18T01:02:44Z","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":"Multi-gap RPC prototypes with readout on a multi-strip electrode were developed for the small polar angle region of the CBM-TOF subdetector, the most demanding zone in terms of granularity and counting rate. The prototypes are based on low resistivity ($\\sim$10$^{10}$ $\\Omega$cm) glass electrodes for performing in high counting rate environment. The strip width/pitch size was chosen such to fulfill the impedance matching with the front-end electronics and the granularity requirements of the innermost zone of the CBM-TOF wall. The in-beam tests using secondary particles produced in heavy ion co","authors_text":"C. Simon, D. Barto\\c{s}, G. Caragheorgheopol, I. Deppner, J. Fr\\\"uhauf, L. R\\v{a}dulescu, M. Ki\\v{s}, M. Petri\\c{s}, M. Petrovici, N. Herrmann, P-A. Loizeau, V. Simion","cross_cats":["hep-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-05-09T12:37:19Z","title":"Time and position resolution of high granularity, high counting rate MRPC for the inner zone of the CBM-TOF wall"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.02558","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:e4913ec9e7d8b03b9630b0f0ae916f1a24487e3e7cb132f87660b15becf141df","target":"record","created_at":"2026-05-18T01:02:44Z","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":"727b4982e559dadb4508bde20959da7bb72244db3f962b91b7438e895aa4b0b6","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-05-09T12:37:19Z","title_canon_sha256":"b237c1dbb6f7d1329684e36c3c1e20d80950256f0bdf18abc26e0403f7055282"},"schema_version":"1.0","source":{"id":"1605.02558","kind":"arxiv","version":1}},"canonical_sha256":"f9b970c02febf58406898bf80b5c2f5f64af11bdfb23dcd6c28a53cc1b4ad03f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f9b970c02febf58406898bf80b5c2f5f64af11bdfb23dcd6c28a53cc1b4ad03f","first_computed_at":"2026-05-18T01:02:44.253836Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:02:44.253836Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2nBLjId+n/QTd4zo09HqGAXWSBDrM6gpDWO92t1moGar2Mh6FdY/1cORlxkGx2v/KCH2P6fFVppF3KGXWiTBCA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:02:44.254256Z","signed_message":"canonical_sha256_bytes"},"source_id":"1605.02558","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e4913ec9e7d8b03b9630b0f0ae916f1a24487e3e7cb132f87660b15becf141df","sha256:55a350b26d05dea57b7184e550037858e65f995691b0fce2423e21fad7d516ac"],"state_sha256":"d641927f6360fa6d11b6ce32907cde52bd07c412fc199ad29b0c928e82185d92"}