{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:PGI4ISLGEHFUFVQ7SP3Q63RBWT","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":"66e69c2c729fbe309a07abd47302c6b36c259aaa565a21fb979e3e2d68632eaa","cross_cats_sorted":["astro-ph.EP","physics.space-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2022-11-10T07:58:40Z","title_canon_sha256":"3acaa89a765d0c554661828812434590833e4374c39d09c66233d513c4c2cd12"},"schema_version":"1.0","source":{"id":"2211.05398","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2211.05398","created_at":"2026-07-05T05:48:42Z"},{"alias_kind":"arxiv_version","alias_value":"2211.05398v1","created_at":"2026-07-05T05:48:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2211.05398","created_at":"2026-07-05T05:48:42Z"},{"alias_kind":"pith_short_12","alias_value":"PGI4ISLGEHFU","created_at":"2026-07-05T05:48:42Z"},{"alias_kind":"pith_short_16","alias_value":"PGI4ISLGEHFUFVQ7","created_at":"2026-07-05T05:48:42Z"},{"alias_kind":"pith_short_8","alias_value":"PGI4ISLG","created_at":"2026-07-05T05:48:42Z"}],"graph_snapshots":[{"event_id":"sha256:2afc69ba8f24fcc7fdfc94d038e4653f3a68ec21192ac96e9d722d00b76baaf6","target":"graph","created_at":"2026-07-05T05:48:42Z","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/2211.05398/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Thermalization and heating of plasma flows at shocks result in unstable charged-particle distributions which generate a wide range of electromagnetic waves. These waves, in turn, can further accelerate and scatter energetic particles. Thus, the properties of the waves and their implication for wave-particle interactions are critically important for modeling energetic particle dynamics in shock environments. Whistler-mode waves, excited by the electron heat flux or a temperature anisotropy, arise naturally near shocks and foreshock transients. As a result, they can often interact with supra-the","authors_text":"Anton Artemyev, Drew L. Turner, Terry Liu, Vassilis Angelopoulos, Xiaofei Shi, Xiao-Jia Zhang","cross_cats":["astro-ph.EP","physics.space-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2022-11-10T07:58:40Z","title":"Intense whistler-mode waves at foreshock transients: characteristics and regimes of wave-particle resonant interaction"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2211.05398","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":"sha256:826eb0f5042eaa548d545120946a8ae586eea456d5957adcbc445b99f76c4fb5","target":"record","created_at":"2026-07-05T05:48:42Z","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":"66e69c2c729fbe309a07abd47302c6b36c259aaa565a21fb979e3e2d68632eaa","cross_cats_sorted":["astro-ph.EP","physics.space-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2022-11-10T07:58:40Z","title_canon_sha256":"3acaa89a765d0c554661828812434590833e4374c39d09c66233d513c4c2cd12"},"schema_version":"1.0","source":{"id":"2211.05398","kind":"arxiv","version":1}},"canonical_sha256":"7991c4496621cb42d61f93f70f6e21b4d3ac57bab54afe20e147da3245305b17","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7991c4496621cb42d61f93f70f6e21b4d3ac57bab54afe20e147da3245305b17","first_computed_at":"2026-07-05T05:48:42.150606Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:48:42.150606Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"3A7gQ5fs6UT4/TEBkoC7WzZxxXXO1mG2SqibDPaBVIPsjATH5jrIpa7WsnabEQ9Pgl4RvgZcXW4ZixgzF3eICw==","signature_status":"signed_v1","signed_at":"2026-07-05T05:48:42.151088Z","signed_message":"canonical_sha256_bytes"},"source_id":"2211.05398","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:826eb0f5042eaa548d545120946a8ae586eea456d5957adcbc445b99f76c4fb5","sha256:2afc69ba8f24fcc7fdfc94d038e4653f3a68ec21192ac96e9d722d00b76baaf6"],"state_sha256":"a0e9261ef5fe2629f834c8626c52b3c9df12ce43e9c27d8e8ec67ae691a787fa"}