{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:YACHSZOS7V6M6RIBKNBYXL6KOF","short_pith_number":"pith:YACHSZOS","schema_version":"1.0","canonical_sha256":"c0047965d2fd7ccf450153438bafca715eed8ccda8194182efdd289c17f81584","source":{"kind":"arxiv","id":"1003.5951","version":1},"attestation_state":"computed","paper":{"title":"Scaling laws of resistive magnetohydrodynamic reconnection in the high-Lundquist-number, plasmoid-unstable regime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.SR"],"primary_cat":"physics.plasm-ph","authors_text":"A. Bhattacharjee, Yi-Min Huang","submitted_at":"2010-03-30T23:56:11Z","abstract_excerpt":"The Sweet-Parker layer in a system that exceeds a critical value of the Lundquist number ($S$) is unstable to the plasmoid instability. In this paper, a numerical scaling study has been done with an island coalescing system driven by a low level of random noise. In the early stage, a primary Sweet-Parker layer forms between the two coalescing islands. The primary Sweet-Parker layer breaks into multiple plasmoids and even thinner current sheets through multiple levels of cascading if the Lundquist number is greater than a critical value $S_{c}\\simeq4\\times10^{4}$. As a result of the plasmoid in"},"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":"1003.5951","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2010-03-30T23:56:11Z","cross_cats_sorted":["astro-ph.SR"],"title_canon_sha256":"8653fb3b84d1234e4c1058bdf91f9eb3810d2005585ecc4b1b277a8e3db93c66","abstract_canon_sha256":"bb66c8472f48affb66e70a379115395768e217e1a4ccc15739ad80d86ba0b629"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:24:25.861050Z","signature_b64":"EG+BzAUQsrCjkVRsM2GY/H20h1SSSQRQtLVDjCdiAw2Ia39pBRqnCMDi/txgKU8oiyvgN3/B5ScTaN4MRy6uDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c0047965d2fd7ccf450153438bafca715eed8ccda8194182efdd289c17f81584","last_reissued_at":"2026-05-18T02:24:25.860379Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:24:25.860379Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Scaling laws of resistive magnetohydrodynamic reconnection in the high-Lundquist-number, plasmoid-unstable regime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.SR"],"primary_cat":"physics.plasm-ph","authors_text":"A. Bhattacharjee, Yi-Min Huang","submitted_at":"2010-03-30T23:56:11Z","abstract_excerpt":"The Sweet-Parker layer in a system that exceeds a critical value of the Lundquist number ($S$) is unstable to the plasmoid instability. In this paper, a numerical scaling study has been done with an island coalescing system driven by a low level of random noise. In the early stage, a primary Sweet-Parker layer forms between the two coalescing islands. The primary Sweet-Parker layer breaks into multiple plasmoids and even thinner current sheets through multiple levels of cascading if the Lundquist number is greater than a critical value $S_{c}\\simeq4\\times10^{4}$. As a result of the plasmoid in"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1003.5951","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":""},"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":"1003.5951","created_at":"2026-05-18T02:24:25.860465+00:00"},{"alias_kind":"arxiv_version","alias_value":"1003.5951v1","created_at":"2026-05-18T02:24:25.860465+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1003.5951","created_at":"2026-05-18T02:24:25.860465+00:00"},{"alias_kind":"pith_short_12","alias_value":"YACHSZOS7V6M","created_at":"2026-05-18T12:26:17.028572+00:00"},{"alias_kind":"pith_short_16","alias_value":"YACHSZOS7V6M6RIB","created_at":"2026-05-18T12:26:17.028572+00:00"},{"alias_kind":"pith_short_8","alias_value":"YACHSZOS","created_at":"2026-05-18T12:26:17.028572+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.18946","citing_title":"Magnetic Prandtl number dependence of plasmoid-mediated reconnection","ref_index":13,"is_internal_anchor":true},{"citing_arxiv_id":"2605.06085","citing_title":"Tearing of charged current layers","ref_index":15,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/YACHSZOS7V6M6RIBKNBYXL6KOF","json":"https://pith.science/pith/YACHSZOS7V6M6RIBKNBYXL6KOF.json","graph_json":"https://pith.science/api/pith-number/YACHSZOS7V6M6RIBKNBYXL6KOF/graph.json","events_json":"https://pith.science/api/pith-number/YACHSZOS7V6M6RIBKNBYXL6KOF/events.json","paper":"https://pith.science/paper/YACHSZOS"},"agent_actions":{"view_html":"https://pith.science/pith/YACHSZOS7V6M6RIBKNBYXL6KOF","download_json":"https://pith.science/pith/YACHSZOS7V6M6RIBKNBYXL6KOF.json","view_paper":"https://pith.science/paper/YACHSZOS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1003.5951&json=true","fetch_graph":"https://pith.science/api/pith-number/YACHSZOS7V6M6RIBKNBYXL6KOF/graph.json","fetch_events":"https://pith.science/api/pith-number/YACHSZOS7V6M6RIBKNBYXL6KOF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YACHSZOS7V6M6RIBKNBYXL6KOF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YACHSZOS7V6M6RIBKNBYXL6KOF/action/storage_attestation","attest_author":"https://pith.science/pith/YACHSZOS7V6M6RIBKNBYXL6KOF/action/author_attestation","sign_citation":"https://pith.science/pith/YACHSZOS7V6M6RIBKNBYXL6KOF/action/citation_signature","submit_replication":"https://pith.science/pith/YACHSZOS7V6M6RIBKNBYXL6KOF/action/replication_record"}},"created_at":"2026-05-18T02:24:25.860465+00:00","updated_at":"2026-05-18T02:24:25.860465+00:00"}