{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:CIUCSJPQEAJNAYMBDKSV7BRJW5","short_pith_number":"pith:CIUCSJPQ","schema_version":"1.0","canonical_sha256":"12282925f02012d061811aa55f8629b7625b7776c26a0a215eb5c27545c86df0","source":{"kind":"arxiv","id":"2501.17601","version":1},"attestation_state":"computed","paper":{"title":"Electron dynamics of three distinct discharge modes of a cross-field atmospheric pressure plasma jet","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"David Alexander Schulenberg, Ihor Korolov, Julian Schulze, Mate Vass, Maximilian Klich, Ralf Peter Brinkmann, Sebastian Wilczek, Thomas Mussenbrock, Tim Bolles","submitted_at":"2025-01-29T12:11:23Z","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"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2501.17601","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-01-29T12:11:23Z","cross_cats_sorted":[],"title_canon_sha256":"f0bf1916b2c04843fa4b7491233021d995bb30ded7fee3bda2e18381c069cc7a","abstract_canon_sha256":"9a46024266c3b1810bed561927cae68a94e302038b0b4ceabe98952aaac7ceaa"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:06:55.608373Z","signature_b64":"IyYoPsVN1YQ2yH1K/TK1bAo32fT/7FQdFNIPf4+0R1l8kLSaN2oEnZjZpiufoH9ADZPE1pWzS9q2v4WY9VeiAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"12282925f02012d061811aa55f8629b7625b7776c26a0a215eb5c27545c86df0","last_reissued_at":"2026-07-05T10:06:55.607848Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:06:55.607848Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electron dynamics of three distinct discharge modes of a cross-field atmospheric pressure plasma jet","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"David Alexander Schulenberg, Ihor Korolov, Julian Schulze, Mate Vass, Maximilian Klich, Ralf Peter Brinkmann, Sebastian Wilczek, Thomas Mussenbrock, Tim Bolles","submitted_at":"2025-01-29T12:11:23Z","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"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2501.17601","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2501.17601/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2501.17601","created_at":"2026-07-05T10:06:55.607918+00:00"},{"alias_kind":"arxiv_version","alias_value":"2501.17601v1","created_at":"2026-07-05T10:06:55.607918+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.17601","created_at":"2026-07-05T10:06:55.607918+00:00"},{"alias_kind":"pith_short_12","alias_value":"CIUCSJPQEAJN","created_at":"2026-07-05T10:06:55.607918+00:00"},{"alias_kind":"pith_short_16","alias_value":"CIUCSJPQEAJNAYMB","created_at":"2026-07-05T10:06:55.607918+00:00"},{"alias_kind":"pith_short_8","alias_value":"CIUCSJPQ","created_at":"2026-07-05T10:06:55.607918+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CIUCSJPQEAJNAYMBDKSV7BRJW5","json":"https://pith.science/pith/CIUCSJPQEAJNAYMBDKSV7BRJW5.json","graph_json":"https://pith.science/api/pith-number/CIUCSJPQEAJNAYMBDKSV7BRJW5/graph.json","events_json":"https://pith.science/api/pith-number/CIUCSJPQEAJNAYMBDKSV7BRJW5/events.json","paper":"https://pith.science/paper/CIUCSJPQ"},"agent_actions":{"view_html":"https://pith.science/pith/CIUCSJPQEAJNAYMBDKSV7BRJW5","download_json":"https://pith.science/pith/CIUCSJPQEAJNAYMBDKSV7BRJW5.json","view_paper":"https://pith.science/paper/CIUCSJPQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2501.17601&json=true","fetch_graph":"https://pith.science/api/pith-number/CIUCSJPQEAJNAYMBDKSV7BRJW5/graph.json","fetch_events":"https://pith.science/api/pith-number/CIUCSJPQEAJNAYMBDKSV7BRJW5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CIUCSJPQEAJNAYMBDKSV7BRJW5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CIUCSJPQEAJNAYMBDKSV7BRJW5/action/storage_attestation","attest_author":"https://pith.science/pith/CIUCSJPQEAJNAYMBDKSV7BRJW5/action/author_attestation","sign_citation":"https://pith.science/pith/CIUCSJPQEAJNAYMBDKSV7BRJW5/action/citation_signature","submit_replication":"https://pith.science/pith/CIUCSJPQEAJNAYMBDKSV7BRJW5/action/replication_record"}},"created_at":"2026-07-05T10:06:55.607918+00:00","updated_at":"2026-07-05T10:06:55.607918+00:00"}