{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:HT6EJROUL6FI6L4AP5UUJ4MXEW","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":"fa7a4e5cb5130e27b300b8fcd6b701e7896754e430b74efb0da8bfaa7cf9171a","cross_cats_sorted":["physics.plasm-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.space-ph","submitted_at":"2021-10-16T05:44:16Z","title_canon_sha256":"c7b05cdc3300e9e3dda500a80b80993eccd2ed1cb31da568174fc21b00e2344e"},"schema_version":"1.0","source":{"id":"2110.08478","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2110.08478","created_at":"2026-07-05T03:36:16Z"},{"alias_kind":"arxiv_version","alias_value":"2110.08478v1","created_at":"2026-07-05T03:36:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2110.08478","created_at":"2026-07-05T03:36:16Z"},{"alias_kind":"pith_short_12","alias_value":"HT6EJROUL6FI","created_at":"2026-07-05T03:36:16Z"},{"alias_kind":"pith_short_16","alias_value":"HT6EJROUL6FI6L4A","created_at":"2026-07-05T03:36:16Z"},{"alias_kind":"pith_short_8","alias_value":"HT6EJROU","created_at":"2026-07-05T03:36:16Z"}],"graph_snapshots":[{"event_id":"sha256:1924e56c49688595d340f890f2e41ee9603707f0cd4df7bdea046d8b7ba119ca","target":"graph","created_at":"2026-07-05T03:36:16Z","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/2110.08478/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"One of the most important problems of magnetotail dynamics is the substorm onset and the related instability of the magneotail current sheet. Since the simplest 2D current sheet configuration with monotonic $B_z$ was proven to be stable to the tearing mode, the focus of the instability investigation moved to more specific configurations, e.g. kinetic current sheets with strong transient ion currents and current sheets with non-monotonic $B_z$ (local $B_z$ minima or/and peaks). Stability of the latter current sheet configuration has been studied both within kinetic and fluid approaches, whereas","authors_text":"Anna Tenerani, Anton Artemyev, Chen Shi, Marco Velli","cross_cats":["physics.plasm-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.space-ph","submitted_at":"2021-10-16T05:44:16Z","title":"Stability of the magnetotail current sheet with normal magnetic field and field-aligned plasma flows"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2110.08478","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":"sha256:7c027de8200c93b478976e1df54b2f57e9bc4e187db0782fea98145d849a8195","target":"record","created_at":"2026-07-05T03:36:16Z","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":"fa7a4e5cb5130e27b300b8fcd6b701e7896754e430b74efb0da8bfaa7cf9171a","cross_cats_sorted":["physics.plasm-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.space-ph","submitted_at":"2021-10-16T05:44:16Z","title_canon_sha256":"c7b05cdc3300e9e3dda500a80b80993eccd2ed1cb31da568174fc21b00e2344e"},"schema_version":"1.0","source":{"id":"2110.08478","kind":"arxiv","version":1}},"canonical_sha256":"3cfc44c5d45f8a8f2f807f6944f19725b0517e12651bb72048d1da0f445f7659","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3cfc44c5d45f8a8f2f807f6944f19725b0517e12651bb72048d1da0f445f7659","first_computed_at":"2026-07-05T03:36:16.649977Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T03:36:16.649977Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"f9f3uTsHCmU6EPFt9XW+1xdZ5RO2BPnOdtmFh1sb/hODbr7lfb8+mTezRNY+aEU7GtCbnzfuGjom8N8gW/fHDg==","signature_status":"signed_v1","signed_at":"2026-07-05T03:36:16.650475Z","signed_message":"canonical_sha256_bytes"},"source_id":"2110.08478","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7c027de8200c93b478976e1df54b2f57e9bc4e187db0782fea98145d849a8195","sha256:1924e56c49688595d340f890f2e41ee9603707f0cd4df7bdea046d8b7ba119ca"],"state_sha256":"3ee706d41537d9b3d88bd2ec07b23411d32740afb710ad08c64303bf54b2788c"}