{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:CIUCSJPQEAJNAYMBDKSV7BRJW5","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":"9a46024266c3b1810bed561927cae68a94e302038b0b4ceabe98952aaac7ceaa","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-01-29T12:11:23Z","title_canon_sha256":"f0bf1916b2c04843fa4b7491233021d995bb30ded7fee3bda2e18381c069cc7a"},"schema_version":"1.0","source":{"id":"2501.17601","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2501.17601","created_at":"2026-07-05T10:06:55Z"},{"alias_kind":"arxiv_version","alias_value":"2501.17601v1","created_at":"2026-07-05T10:06:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.17601","created_at":"2026-07-05T10:06:55Z"},{"alias_kind":"pith_short_12","alias_value":"CIUCSJPQEAJN","created_at":"2026-07-05T10:06:55Z"},{"alias_kind":"pith_short_16","alias_value":"CIUCSJPQEAJNAYMB","created_at":"2026-07-05T10:06:55Z"},{"alias_kind":"pith_short_8","alias_value":"CIUCSJPQ","created_at":"2026-07-05T10:06:55Z"}],"graph_snapshots":[{"event_id":"sha256:bdcfd9c995fda28e6fdac99f380efafe0b4782048d5a4d467cbe9de3b0d7f3ad","target":"graph","created_at":"2026-07-05T10:06:55Z","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/2501.17601/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"This paper investigates the electron dynamics in three distinct discharge modes of a cross-field atmospheric pressure plasma jet, the COST-Jet. Thereby, the discharge modes are the non-neutral, the quasi-neutral, and the constricted mode. Using a hybrid Particle-In-Cell/Monte-Carlo Collisions (PIC/MCC) simulation, the study systematically varies the applied voltage and driving frequency to explore the operation modes and their relations. The results reveal that at low input power, the COST-Jet operates in a non-neutral mode, characterized by a discharge close to extinction, analogous to the ch","authors_text":"David Alexander Schulenberg, Ihor Korolov, Julian Schulze, Mate Vass, Maximilian Klich, Ralf Peter Brinkmann, Sebastian Wilczek, Thomas Mussenbrock, Tim Bolles","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-01-29T12:11:23Z","title":"Electron dynamics of three distinct discharge modes of a cross-field atmospheric pressure plasma jet"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2501.17601","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":"sha256:0f36f6a3b883457777ed6ef48c4a504f980cf57feacd50a44d2d1d9a775bf0c8","target":"record","created_at":"2026-07-05T10:06:55Z","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":"9a46024266c3b1810bed561927cae68a94e302038b0b4ceabe98952aaac7ceaa","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-01-29T12:11:23Z","title_canon_sha256":"f0bf1916b2c04843fa4b7491233021d995bb30ded7fee3bda2e18381c069cc7a"},"schema_version":"1.0","source":{"id":"2501.17601","kind":"arxiv","version":1}},"canonical_sha256":"12282925f02012d061811aa55f8629b7625b7776c26a0a215eb5c27545c86df0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"12282925f02012d061811aa55f8629b7625b7776c26a0a215eb5c27545c86df0","first_computed_at":"2026-07-05T10:06:55.607848Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:06:55.607848Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"IyYoPsVN1YQ2yH1K/TK1bAo32fT/7FQdFNIPf4+0R1l8kLSaN2oEnZjZpiufoH9ADZPE1pWzS9q2v4WY9VeiAQ==","signature_status":"signed_v1","signed_at":"2026-07-05T10:06:55.608373Z","signed_message":"canonical_sha256_bytes"},"source_id":"2501.17601","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0f36f6a3b883457777ed6ef48c4a504f980cf57feacd50a44d2d1d9a775bf0c8","sha256:bdcfd9c995fda28e6fdac99f380efafe0b4782048d5a4d467cbe9de3b0d7f3ad"],"state_sha256":"db876f61fd7e177e867351b1502841f0616b66879aa999ba612ba14c139b9be4"}