{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:6QC6LMV5ENGYJHKAXYD762RWBT","short_pith_number":"pith:6QC6LMV5","schema_version":"1.0","canonical_sha256":"f405e5b2bd234d849d40be07ff6a360ce38cc2931a87a714bd7e0917e61ddc96","source":{"kind":"arxiv","id":"1609.04935","version":1},"attestation_state":"computed","paper":{"title":"How do the barrier thickness and dielectric material influence the filamentary mode and CO2 conversion in a flowing DBD?","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"A Bogaerts, A Ozkan, F Reniers, Thierry Dufour","submitted_at":"2016-09-16T08:06:02Z","abstract_excerpt":"Dielectric barrier discharges (DBDs) are commonly used to generate cold plasmas at atmospheric pressure. Whatever their configuration (tubular or planar), the presence of a dielectric barrier is mandatory to prevent too much charge build up in the plasma and the formation of a thermal arc. In this article, the role of the barrier thickness (2.0, 2.4 and 2.8 mm) and of the kind of dielectric material (alumina, mullite, pyrex, quartz) is investigated on the filamentary behavior in the plasma and on the CO2 conversion in a tubular flowing DBD, by means of mass spectrometry measurements correlated"},"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":"1609.04935","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2016-09-16T08:06:02Z","cross_cats_sorted":[],"title_canon_sha256":"d5a9ebecf11e8de96ae772192dfad319c4e6b768902ab8c7c5551b8902b092a4","abstract_canon_sha256":"9c9539b2ab5b7355574b228ad6f84ad02efc30567f109a75be277ae822e27ad7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:04:32.025961Z","signature_b64":"vBnWf5RPHMnk6iMB8aEwZn5t6mVz/Iap/0yqCho0yrEY9Sn5kEYg8kbXUzDR0z+0I0EroR49YBn5kViDSPgvAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f405e5b2bd234d849d40be07ff6a360ce38cc2931a87a714bd7e0917e61ddc96","last_reissued_at":"2026-05-18T01:04:32.025152Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:04:32.025152Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"How do the barrier thickness and dielectric material influence the filamentary mode and CO2 conversion in a flowing DBD?","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"A Bogaerts, A Ozkan, F Reniers, Thierry Dufour","submitted_at":"2016-09-16T08:06:02Z","abstract_excerpt":"Dielectric barrier discharges (DBDs) are commonly used to generate cold plasmas at atmospheric pressure. Whatever their configuration (tubular or planar), the presence of a dielectric barrier is mandatory to prevent too much charge build up in the plasma and the formation of a thermal arc. In this article, the role of the barrier thickness (2.0, 2.4 and 2.8 mm) and of the kind of dielectric material (alumina, mullite, pyrex, quartz) is investigated on the filamentary behavior in the plasma and on the CO2 conversion in a tubular flowing DBD, by means of mass spectrometry measurements correlated"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.04935","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":""},"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":"1609.04935","created_at":"2026-05-18T01:04:32.025286+00:00"},{"alias_kind":"arxiv_version","alias_value":"1609.04935v1","created_at":"2026-05-18T01:04:32.025286+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.04935","created_at":"2026-05-18T01:04:32.025286+00:00"},{"alias_kind":"pith_short_12","alias_value":"6QC6LMV5ENGY","created_at":"2026-05-18T12:30:01.593930+00:00"},{"alias_kind":"pith_short_16","alias_value":"6QC6LMV5ENGYJHKA","created_at":"2026-05-18T12:30:01.593930+00:00"},{"alias_kind":"pith_short_8","alias_value":"6QC6LMV5","created_at":"2026-05-18T12:30:01.593930+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/6QC6LMV5ENGYJHKAXYD762RWBT","json":"https://pith.science/pith/6QC6LMV5ENGYJHKAXYD762RWBT.json","graph_json":"https://pith.science/api/pith-number/6QC6LMV5ENGYJHKAXYD762RWBT/graph.json","events_json":"https://pith.science/api/pith-number/6QC6LMV5ENGYJHKAXYD762RWBT/events.json","paper":"https://pith.science/paper/6QC6LMV5"},"agent_actions":{"view_html":"https://pith.science/pith/6QC6LMV5ENGYJHKAXYD762RWBT","download_json":"https://pith.science/pith/6QC6LMV5ENGYJHKAXYD762RWBT.json","view_paper":"https://pith.science/paper/6QC6LMV5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1609.04935&json=true","fetch_graph":"https://pith.science/api/pith-number/6QC6LMV5ENGYJHKAXYD762RWBT/graph.json","fetch_events":"https://pith.science/api/pith-number/6QC6LMV5ENGYJHKAXYD762RWBT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6QC6LMV5ENGYJHKAXYD762RWBT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6QC6LMV5ENGYJHKAXYD762RWBT/action/storage_attestation","attest_author":"https://pith.science/pith/6QC6LMV5ENGYJHKAXYD762RWBT/action/author_attestation","sign_citation":"https://pith.science/pith/6QC6LMV5ENGYJHKAXYD762RWBT/action/citation_signature","submit_replication":"https://pith.science/pith/6QC6LMV5ENGYJHKAXYD762RWBT/action/replication_record"}},"created_at":"2026-05-18T01:04:32.025286+00:00","updated_at":"2026-05-18T01:04:32.025286+00:00"}