{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:4QJKIRAWDNEON4MPUO2XMVYK5F","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":"0cdb9076b8b2d0836c347c8c2bd7ee4ca680c86592f06a5a9dcc6b1581f446b5","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2017-10-18T14:56:58Z","title_canon_sha256":"d9b823eae4d617ffbffd41328c0da2d8b4435ba107dfadcf1c24ea6b3731cea9"},"schema_version":"1.0","source":{"id":"1712.01354","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1712.01354","created_at":"2026-05-17T23:51:14Z"},{"alias_kind":"arxiv_version","alias_value":"1712.01354v1","created_at":"2026-05-17T23:51:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1712.01354","created_at":"2026-05-17T23:51:14Z"},{"alias_kind":"pith_short_12","alias_value":"4QJKIRAWDNEO","created_at":"2026-05-18T12:31:00Z"},{"alias_kind":"pith_short_16","alias_value":"4QJKIRAWDNEON4MP","created_at":"2026-05-18T12:31:00Z"},{"alias_kind":"pith_short_8","alias_value":"4QJKIRAW","created_at":"2026-05-18T12:31:00Z"}],"graph_snapshots":[{"event_id":"sha256:c46259316a12ebfc060975eee503e05f862289f5ca150b399f30484ec8234f36","target":"graph","created_at":"2026-05-17T23:51:14Z","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 1T polytype of TaS2 exhibits voltage-triggered threshold switching as a result of a phase transition from nearly commensurate to incommensurate charge density wave states. Threshold switching, persistent above room temperature, can be utilized in a variety of electronic devices, e.g., voltage controlled oscillators. We evaluated the total-ionizing-dose response of thin film 1T-TaS2 at doses up to 1 Mrad(SiO2). The threshold voltage changed by less than 2% after irradiation, with persistent self-sustained oscillations observed through the full irradiation sequence. The radiation hardness is","authors_text":"A.A. Balandin, C. D. Liang, D.M. Fleetwood, E. X. Zhang, G. Liu, M.A. Bloodgood, T.T. Salguero","cross_cats":["cond-mat.mes-hall"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2017-10-18T14:56:58Z","title":"Total Ionizing Dose Effects on Threshold Switching in 1T-Tantalum Disulfide Charge-Density-Wave Devices"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1712.01354","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":"sha256:1d047bf7d60162025d6a040c2d9574f1691eaaff9e6fd15129e5f5e2784b09c9","target":"record","created_at":"2026-05-17T23:51:14Z","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":"0cdb9076b8b2d0836c347c8c2bd7ee4ca680c86592f06a5a9dcc6b1581f446b5","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2017-10-18T14:56:58Z","title_canon_sha256":"d9b823eae4d617ffbffd41328c0da2d8b4435ba107dfadcf1c24ea6b3731cea9"},"schema_version":"1.0","source":{"id":"1712.01354","kind":"arxiv","version":1}},"canonical_sha256":"e412a444161b48e6f18fa3b576570ae950772672e69169129114ade4840b770e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e412a444161b48e6f18fa3b576570ae950772672e69169129114ade4840b770e","first_computed_at":"2026-05-17T23:51:14.763508Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:51:14.763508Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"MspUCB+EKUk1e5DCukmaJYyDHuQY24msDf+OvMX+WWc2KtFhPsAm2uXgfG/vzvbqISV6pV+oI3hy71uLNr3nDA==","signature_status":"signed_v1","signed_at":"2026-05-17T23:51:14.764177Z","signed_message":"canonical_sha256_bytes"},"source_id":"1712.01354","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1d047bf7d60162025d6a040c2d9574f1691eaaff9e6fd15129e5f5e2784b09c9","sha256:c46259316a12ebfc060975eee503e05f862289f5ca150b399f30484ec8234f36"],"state_sha256":"a37db4851c7ac6e103877330b3d13cea1000b6563148257988e97e04b6d79ec7"}