{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:FGFHGZ7PWP26K63OKUS7GKXED6","short_pith_number":"pith:FGFHGZ7P","schema_version":"1.0","canonical_sha256":"298a7367efb3f5e57b6e5525f32ae41fae4cbedfc7d10835198ae3b5d360fc62","source":{"kind":"arxiv","id":"2209.00149","version":1},"attestation_state":"computed","paper":{"title":"A New Approach of Linear Theory of Tearing Instability in Uniform Resistivity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.SR"],"primary_cat":"physics.plasm-ph","authors_text":"Koji Kondoh, Tohru Shimizu","submitted_at":"2022-08-31T22:51:29Z","abstract_excerpt":"The linear perturbation equation of the tearing instability derived in LSC theory (Loureiro, Schekochihin, and Cowley, PoP2007) is numerically examined as an initial value problem, where the inner and outer regions are seamlessly solved under uniform resistivity. Hence, all regions are solved as the resistive MHD (magnetohydrodynamics). To comprehensively study physically acceptable perturbation solutions, the behaviors of the local maximum points required for physically acceptable solutions and zero-crossing points, at which \\phi=0 and \\psi=0, are examined. Eventually, the uniform resistivity"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2209.00149","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2022-08-31T22:51:29Z","cross_cats_sorted":["astro-ph.SR"],"title_canon_sha256":"cffad69e86ffd10b773626661b2e7bd1ffb1f8e32bc97e96db11b60f7a9cd64c","abstract_canon_sha256":"8f6ac375d17b30fd17e8e5dbd49449d64f3cfa248265c6319b548b655edfb209"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:53:46.452042Z","signature_b64":"NmZl9qnu1tTZ1bKpzqGMPkxxTk2sy2ChD5OCGSKSm3OegglTHTEG/YFLxasR3qV+5rbsrCDtl0VrPM+ccMfuBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"298a7367efb3f5e57b6e5525f32ae41fae4cbedfc7d10835198ae3b5d360fc62","last_reissued_at":"2026-07-05T04:53:46.451599Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:53:46.451599Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A New Approach of Linear Theory of Tearing Instability in Uniform Resistivity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.SR"],"primary_cat":"physics.plasm-ph","authors_text":"Koji Kondoh, Tohru Shimizu","submitted_at":"2022-08-31T22:51:29Z","abstract_excerpt":"The linear perturbation equation of the tearing instability derived in LSC theory (Loureiro, Schekochihin, and Cowley, PoP2007) is numerically examined as an initial value problem, where the inner and outer regions are seamlessly solved under uniform resistivity. Hence, all regions are solved as the resistive MHD (magnetohydrodynamics). To comprehensively study physically acceptable perturbation solutions, the behaviors of the local maximum points required for physically acceptable solutions and zero-crossing points, at which \\phi=0 and \\psi=0, are examined. Eventually, the uniform resistivity"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2209.00149","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2209.00149/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2209.00149","created_at":"2026-07-05T04:53:46.451655+00:00"},{"alias_kind":"arxiv_version","alias_value":"2209.00149v1","created_at":"2026-07-05T04:53:46.451655+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2209.00149","created_at":"2026-07-05T04:53:46.451655+00:00"},{"alias_kind":"pith_short_12","alias_value":"FGFHGZ7PWP26","created_at":"2026-07-05T04:53:46.451655+00:00"},{"alias_kind":"pith_short_16","alias_value":"FGFHGZ7PWP26K63O","created_at":"2026-07-05T04:53:46.451655+00:00"},{"alias_kind":"pith_short_8","alias_value":"FGFHGZ7P","created_at":"2026-07-05T04:53:46.451655+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.00255","citing_title":"Dynamics and Energetics of Resistive, Thermally Conductive, and Radiative Plasma in Coronal Current Sheets due to Asymmetric External Perturbation","ref_index":50,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FGFHGZ7PWP26K63OKUS7GKXED6","json":"https://pith.science/pith/FGFHGZ7PWP26K63OKUS7GKXED6.json","graph_json":"https://pith.science/api/pith-number/FGFHGZ7PWP26K63OKUS7GKXED6/graph.json","events_json":"https://pith.science/api/pith-number/FGFHGZ7PWP26K63OKUS7GKXED6/events.json","paper":"https://pith.science/paper/FGFHGZ7P"},"agent_actions":{"view_html":"https://pith.science/pith/FGFHGZ7PWP26K63OKUS7GKXED6","download_json":"https://pith.science/pith/FGFHGZ7PWP26K63OKUS7GKXED6.json","view_paper":"https://pith.science/paper/FGFHGZ7P","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2209.00149&json=true","fetch_graph":"https://pith.science/api/pith-number/FGFHGZ7PWP26K63OKUS7GKXED6/graph.json","fetch_events":"https://pith.science/api/pith-number/FGFHGZ7PWP26K63OKUS7GKXED6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FGFHGZ7PWP26K63OKUS7GKXED6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FGFHGZ7PWP26K63OKUS7GKXED6/action/storage_attestation","attest_author":"https://pith.science/pith/FGFHGZ7PWP26K63OKUS7GKXED6/action/author_attestation","sign_citation":"https://pith.science/pith/FGFHGZ7PWP26K63OKUS7GKXED6/action/citation_signature","submit_replication":"https://pith.science/pith/FGFHGZ7PWP26K63OKUS7GKXED6/action/replication_record"}},"created_at":"2026-07-05T04:53:46.451655+00:00","updated_at":"2026-07-05T04:53:46.451655+00:00"}