{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:2IZCCHRA5LI3GOWWK53GU5OZSG","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":"4be5555db11322b6e13f8167da4db8236aaa414c64f9fe4102be8d26182cb189","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-06-05T06:11:26Z","title_canon_sha256":"904e39de480b8d2d33d3ee9f2c982fc95a8d1db6e700c6a73567e2799c40d033"},"schema_version":"1.0","source":{"id":"1706.01204","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.01204","created_at":"2026-05-18T00:30:22Z"},{"alias_kind":"arxiv_version","alias_value":"1706.01204v1","created_at":"2026-05-18T00:30:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.01204","created_at":"2026-05-18T00:30:22Z"},{"alias_kind":"pith_short_12","alias_value":"2IZCCHRA5LI3","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_16","alias_value":"2IZCCHRA5LI3GOWW","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_8","alias_value":"2IZCCHRA","created_at":"2026-05-18T12:30:55Z"}],"graph_snapshots":[{"event_id":"sha256:1c5f2c614d5e7b4a375497f801e973944c9f3bdb35f7046b941607d160688270","target":"graph","created_at":"2026-05-18T00:30:22Z","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"},"paper":{"abstract_excerpt":"Some low-$n$ kink-ballooning modes not far from marginal stability are shown to exhibit a bifurcation between two very distinct nonlinear paths that depends sensitively on the background transport levels and linear perturbation amplitudes. The particular instability studied in this work is an $n=1$ mode dominated by an $m/n=2/1$ component. It is driven by a large pressure gradient in weak magnetic shear and can appear in various high-$\\beta,$ hybrid/advanced scenarios. Here it is investigated in reversed shear equilibria where the region around the safety-factor minimum provides favorable cond","authors_text":"A. Y. Aydemir, B. H. Park, Y. K. In","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-06-05T06:11:26Z","title":"Dynamics of an $n=1$ explosive instability and its role in high-$\\beta$ disruptions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.01204","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":"sha256:7920a49687c098bc1ddac38b073f25c44d26bec79b2613661d5d74ef982cd55e","target":"record","created_at":"2026-05-18T00:30:22Z","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":"4be5555db11322b6e13f8167da4db8236aaa414c64f9fe4102be8d26182cb189","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-06-05T06:11:26Z","title_canon_sha256":"904e39de480b8d2d33d3ee9f2c982fc95a8d1db6e700c6a73567e2799c40d033"},"schema_version":"1.0","source":{"id":"1706.01204","kind":"arxiv","version":1}},"canonical_sha256":"d232211e20ead1b33ad657766a75d991959b2c47142fc022aa62adcd35c6c85e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d232211e20ead1b33ad657766a75d991959b2c47142fc022aa62adcd35c6c85e","first_computed_at":"2026-05-18T00:30:22.111436Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:30:22.111436Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"oiw9KgC7rVeAJihgIZSVWSdS+2rRi8LNHaNTeedgBVUjbmP/29DWF25HUsKgS1wg+/kRg8kqqxaCPFAwhWB9AA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:30:22.112163Z","signed_message":"canonical_sha256_bytes"},"source_id":"1706.01204","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7920a49687c098bc1ddac38b073f25c44d26bec79b2613661d5d74ef982cd55e","sha256:1c5f2c614d5e7b4a375497f801e973944c9f3bdb35f7046b941607d160688270"],"state_sha256":"ede549394b6ed4e6f2d4db1732ad413124c9b1cbc73fc679c8bdffba888848b6"}