{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:I2VF5KBDVC3PZW7IP4RBOALTPQ","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":"53fbed73ea564824d39239580e98383c25f056a42c050ba95e889c4617965a03","cross_cats_sorted":["physics.comp-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2026-07-22T09:02:05Z","title_canon_sha256":"6fdd189962ad06896a2a80ff525e188b2e23955986cf6b42c5abb1f2d3b5529f"},"schema_version":"1.0","source":{"id":"2607.19930","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2607.19930","created_at":"2026-07-23T01:24:44Z"},{"alias_kind":"arxiv_version","alias_value":"2607.19930v1","created_at":"2026-07-23T01:24:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.19930","created_at":"2026-07-23T01:24:44Z"},{"alias_kind":"pith_short_12","alias_value":"I2VF5KBDVC3P","created_at":"2026-07-23T01:24:44Z"},{"alias_kind":"pith_short_16","alias_value":"I2VF5KBDVC3PZW7I","created_at":"2026-07-23T01:24:44Z"},{"alias_kind":"pith_short_8","alias_value":"I2VF5KBD","created_at":"2026-07-23T01:24:44Z"}],"graph_snapshots":[{"event_id":"sha256:40cc2c9521900ad720dc279b3904eb24928b9232221e34fc0ae598ef3cbe8c83","target":"graph","created_at":"2026-07-23T01:24:44Z","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/2607.19930/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"A reduced-order non-self-consistent Monte Carlo model is presented for a circular planar magnetron discharge in argon. The model combines two magnetic-field representations, namely a superposition of magnetic dipoles and a numerically integrated field of the finite permanent magnets, with a prescribed one-dimensional sheath-bulk potential, adaptive fourth-order Runge-Kutta orbit integration, and a null-collision treatment of electron-argon collisions. The collision module reproduces the dependence of the electron drift velocity on the reduced electric field, but overestimates its absolute valu","authors_text":"Franz F. Locker, Georg Strau{\\ss}","cross_cats":["physics.comp-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2026-07-22T09:02:05Z","title":"Reduced-order non-self-consistent Monte Carlo simulation of a planar magnetron discharge: electron heating, recapture and racetrack formation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.19930","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:b0200d777f705ff603e04b97424a5c70ead2786e9f329c16bda3a9479a54aa5c","target":"record","created_at":"2026-07-23T01:24:44Z","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":"53fbed73ea564824d39239580e98383c25f056a42c050ba95e889c4617965a03","cross_cats_sorted":["physics.comp-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2026-07-22T09:02:05Z","title_canon_sha256":"6fdd189962ad06896a2a80ff525e188b2e23955986cf6b42c5abb1f2d3b5529f"},"schema_version":"1.0","source":{"id":"2607.19930","kind":"arxiv","version":1}},"canonical_sha256":"46aa5ea823a8b6fcdbe87f221701737c358cb8dd14a215692f87f964bb9e76b4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"46aa5ea823a8b6fcdbe87f221701737c358cb8dd14a215692f87f964bb9e76b4","first_computed_at":"2026-07-23T01:24:44.370202Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-23T01:24:44.370202Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"xa/2whHK3Hu/CN49gFgjeBr88vuotHX891KpJc+wWblJRAm6+ZMt18g3fuO1Wd6J33YUAtiBti4WS2/iV6/QAg==","signature_status":"signed_v1","signed_at":"2026-07-23T01:24:44.371042Z","signed_message":"canonical_sha256_bytes"},"source_id":"2607.19930","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b0200d777f705ff603e04b97424a5c70ead2786e9f329c16bda3a9479a54aa5c","sha256:40cc2c9521900ad720dc279b3904eb24928b9232221e34fc0ae598ef3cbe8c83"],"state_sha256":"cf3c69f7406e812ff61ec77f365b0cd01a5798a6d68f44221ca32b7d328c4985"}