{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:QWUIPVFAWCLI7VHWMXH657KAGT","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":"7d396e85b696e065dc46c60fd6288d83756f5dc0f0b6be05739ea8abf81b6d5b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2024-03-01T16:37:34Z","title_canon_sha256":"01bd543c759440282fe630eea40b88247fcca0f48afc6e26f7d9ecd8a53d101c"},"schema_version":"1.0","source":{"id":"2403.00656","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2403.00656","created_at":"2026-07-05T07:51:06Z"},{"alias_kind":"arxiv_version","alias_value":"2403.00656v1","created_at":"2026-07-05T07:51:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2403.00656","created_at":"2026-07-05T07:51:06Z"},{"alias_kind":"pith_short_12","alias_value":"QWUIPVFAWCLI","created_at":"2026-07-05T07:51:06Z"},{"alias_kind":"pith_short_16","alias_value":"QWUIPVFAWCLI7VHW","created_at":"2026-07-05T07:51:06Z"},{"alias_kind":"pith_short_8","alias_value":"QWUIPVFA","created_at":"2026-07-05T07:51:06Z"}],"graph_snapshots":[{"event_id":"sha256:d07cf77ca9fbef748a05c69a9d257a4135e0e42a6c6565f0cd1aeab5f7226341","target":"graph","created_at":"2026-07-05T07:51:06Z","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/2403.00656/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Molecular dynamics simulations are used to test when the particle-in-cell (PIC) method applies to atmospheric pressure plasmas. It is found that PIC applies only when the plasma density and macroparticle weight are sufficiently small because of two effects associated with correlation heating. The first is the physical effect of disorder-induced heating (DIH). This occurs if the plasma density is large enough that a species (typically ions) is strongly correlated in the sense that the Coulomb coupling parameter exceeds one. In this situation, DIH causes ions to rapidly heat following ionization","authors_text":"C. Moore, L. P. Beving, M. Acciarri, S. D. Baalrud","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2024-03-01T16:37:34Z","title":"When should PIC simulations be applied to atmospheric pressure plasmas? Impact of correlation heating"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2403.00656","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:be81e663c6cdb3fdc1d90fc574715b61e28885ddaeec2477415f9be7acb13716","target":"record","created_at":"2026-07-05T07:51:06Z","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":"7d396e85b696e065dc46c60fd6288d83756f5dc0f0b6be05739ea8abf81b6d5b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2024-03-01T16:37:34Z","title_canon_sha256":"01bd543c759440282fe630eea40b88247fcca0f48afc6e26f7d9ecd8a53d101c"},"schema_version":"1.0","source":{"id":"2403.00656","kind":"arxiv","version":1}},"canonical_sha256":"85a887d4a0b0968fd4f665cfeefd4034df577af7011f8dcf12eabcf568178545","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"85a887d4a0b0968fd4f665cfeefd4034df577af7011f8dcf12eabcf568178545","first_computed_at":"2026-07-05T07:51:06.845235Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T07:51:06.845235Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Zm0tbwGd/mSVRriwUE8/lGgWAAGYpQ5UPDGFsHhNsO/zHkQLpDt5UlWAqM+/aPDoW4IXU20NEQeCQbUf/ZQYCw==","signature_status":"signed_v1","signed_at":"2026-07-05T07:51:06.845578Z","signed_message":"canonical_sha256_bytes"},"source_id":"2403.00656","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:be81e663c6cdb3fdc1d90fc574715b61e28885ddaeec2477415f9be7acb13716","sha256:d07cf77ca9fbef748a05c69a9d257a4135e0e42a6c6565f0cd1aeab5f7226341"],"state_sha256":"2cc3695bd7c857f7d3042d20ffa3b87612c4c2d544f23fec3273f40008e413a9"}