{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:OMXIXQBN6XIBNKVOH36PSJVYED","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":"d2c04fcd3fc78e721c8fa6ea22192830c99c5efde203f364182a613248afb815","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-05-25T19:22:32Z","title_canon_sha256":"03e788a910db207792707e093393341d715690f13d437fa67e67aeba47d94499"},"schema_version":"1.0","source":{"id":"2505.19279","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2505.19279","created_at":"2026-07-05T11:09:27Z"},{"alias_kind":"arxiv_version","alias_value":"2505.19279v1","created_at":"2026-07-05T11:09:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.19279","created_at":"2026-07-05T11:09:27Z"},{"alias_kind":"pith_short_12","alias_value":"OMXIXQBN6XIB","created_at":"2026-07-05T11:09:27Z"},{"alias_kind":"pith_short_16","alias_value":"OMXIXQBN6XIBNKVO","created_at":"2026-07-05T11:09:27Z"},{"alias_kind":"pith_short_8","alias_value":"OMXIXQBN","created_at":"2026-07-05T11:09:27Z"}],"graph_snapshots":[{"event_id":"sha256:9c7567dd4aeb7471a3fd4075c3513d69bb738690b52eaaef0436aebb0a2df1ec","target":"graph","created_at":"2026-07-05T11:09:27Z","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/2505.19279/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Helicon waves satisfying the normal wave-particle cyclotron resonance are observed to limit the growth and maximum energy of relativistic electrons (REs) in low-density Ohmic DIII-D tokamak plasmas. Following the application of helicon waves, pitch-angle scattering of high-energy REs causes an increase in both synchrotron and electron-cyclotron emissions. The hard x-ray emission, a proxy for the RE population, ceases to grow; and energy-resolved hard x-ray measurements also show a striking decrease in the number of high-energy REs (above the resonance at approximately \\SI{8}{MeV}) to below the","authors_text":"A. Battey, A. Lvovskiy, B. Van Compernolle, C. Marini, C. Paz-Soldan, D. Spong, H. Choudhury, J. Barr, J. Lestz, N. Leuthold, Q. Zhang, S. Tang, W. Heidbrink, X. Tang, Y. Zhang","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-05-25T19:22:32Z","title":"First Demonstration of Resonant Pitch-Angle Scattering of Relativistic Electrons by Externally-Launched Helicon Waves"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.19279","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:c6bb5ebf55a2b2b9a96d2719046fd5274a6a192d191cba9439be2eb7956d35fd","target":"record","created_at":"2026-07-05T11:09:27Z","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":"d2c04fcd3fc78e721c8fa6ea22192830c99c5efde203f364182a613248afb815","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-05-25T19:22:32Z","title_canon_sha256":"03e788a910db207792707e093393341d715690f13d437fa67e67aeba47d94499"},"schema_version":"1.0","source":{"id":"2505.19279","kind":"arxiv","version":1}},"canonical_sha256":"732e8bc02df5d016aaae3efcf926b820edfb54bff5afad8a822c814c3a612c5e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"732e8bc02df5d016aaae3efcf926b820edfb54bff5afad8a822c814c3a612c5e","first_computed_at":"2026-07-05T11:09:27.463866Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:09:27.463866Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"GBueErfxgpZSkdSV4OIq83MK/BCamoi1giHbEmXK/iPya5CBxCvYarDO1pnJeezjxafOhEnYOoopXk24lH0wDA==","signature_status":"signed_v1","signed_at":"2026-07-05T11:09:27.464368Z","signed_message":"canonical_sha256_bytes"},"source_id":"2505.19279","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c6bb5ebf55a2b2b9a96d2719046fd5274a6a192d191cba9439be2eb7956d35fd","sha256:9c7567dd4aeb7471a3fd4075c3513d69bb738690b52eaaef0436aebb0a2df1ec"],"state_sha256":"6d5a99857206ee555571cc7ddc1845e8ffe86e75115bd17d556efe3182c50d30"}