{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:ZD6ZRURD4ZXBF5VETF3INBP3OR","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":"f81247912c3993b49a9d4572dcbcdbba8b3f8fee1f233598833d3e7dab54fba6","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2019-08-30T09:41:54Z","title_canon_sha256":"ee31859e7f11f88895e16b0105610d52e26d16d08fc20bcf3db27ea88db22738"},"schema_version":"1.0","source":{"id":"1908.11615","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1908.11615","created_at":"2026-07-05T01:11:41Z"},{"alias_kind":"arxiv_version","alias_value":"1908.11615v2","created_at":"2026-07-05T01:11:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1908.11615","created_at":"2026-07-05T01:11:41Z"},{"alias_kind":"pith_short_12","alias_value":"ZD6ZRURD4ZXB","created_at":"2026-07-05T01:11:41Z"},{"alias_kind":"pith_short_16","alias_value":"ZD6ZRURD4ZXBF5VE","created_at":"2026-07-05T01:11:41Z"},{"alias_kind":"pith_short_8","alias_value":"ZD6ZRURD","created_at":"2026-07-05T01:11:41Z"}],"graph_snapshots":[{"event_id":"sha256:dbd4dca347f5f90b868ee83aaa2af9f68110ba8c0cafb2fe782713d2036c7d40","target":"graph","created_at":"2026-07-05T01:11:41Z","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/1908.11615/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"KNOSOS (KiNetic Orbit-averaging SOlver for Stellarators) is a freely available, open-source code (\\href{https://github.com/joseluisvelasco/KNOSOS}{https://github.com/joseluisvelasco/KNOSOS}) that calculates neoclassical transport in low-collisionality plasmas of three-dimensional magnetic confinement devices by solving the radially local drift-kinetic and quasineutrality equations. The main feature of KNOSOS is that it relies on orbit-averaging to solve the drift-kinetic equation very fast. KNOSOS treats rigorously the effect of the component of the magnetic drift that is tangent to magnetic s","authors_text":"F.I. Parra, I. Calvo, J. L. Velasco, J. M. Garc\\'ia-Rega\\~na","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2019-08-30T09:41:54Z","title":"KNOSOS: a fast orbit-averaging neoclassical code for stellarator geometry"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1908.11615","kind":"arxiv","version":2},"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":"sha256:73cea9d2978158b8933952be53e6f15461ed64bd06093a3fa0d947b22b7ca4aa","target":"record","created_at":"2026-07-05T01:11:41Z","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":"f81247912c3993b49a9d4572dcbcdbba8b3f8fee1f233598833d3e7dab54fba6","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2019-08-30T09:41:54Z","title_canon_sha256":"ee31859e7f11f88895e16b0105610d52e26d16d08fc20bcf3db27ea88db22738"},"schema_version":"1.0","source":{"id":"1908.11615","kind":"arxiv","version":2}},"canonical_sha256":"c8fd98d223e66e12f6a499768685fb74736cbe0248c3a8685dc587932ddbaf14","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c8fd98d223e66e12f6a499768685fb74736cbe0248c3a8685dc587932ddbaf14","first_computed_at":"2026-07-05T01:11:41.433588Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T01:11:41.433588Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"9JbGP8CWt1WdlEnOupeCULCwYC2ac+5eX5EsLLjmssh9Dzi0fCtcmsQEmyRybxHtW/YjpkiXOKeqsr2y8lGPDQ==","signature_status":"signed_v1","signed_at":"2026-07-05T01:11:41.434154Z","signed_message":"canonical_sha256_bytes"},"source_id":"1908.11615","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:73cea9d2978158b8933952be53e6f15461ed64bd06093a3fa0d947b22b7ca4aa","sha256:dbd4dca347f5f90b868ee83aaa2af9f68110ba8c0cafb2fe782713d2036c7d40"],"state_sha256":"0371736e823e1d7ad0eb08f56fffb2b4f32696ea051d1fc5e1887039a22a6fd0"}