{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:62NEJWHFIUQVZ3E4MYSOZFQLF6","short_pith_number":"pith:62NEJWHF","schema_version":"1.0","canonical_sha256":"f69a44d8e545215cec9c6624ec960b2f80e6a34f2d8d82ee31c990eab934193b","source":{"kind":"arxiv","id":"1203.2971","version":1},"attestation_state":"computed","paper":{"title":"Reconnection Studies Under Different Types of Turbulence Driving","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.plasm-ph"],"primary_cat":"astro-ph.SR","authors_text":"Alex Lazarian, Ethan T. Vishniac, Grzegorz Kowal, Katarzyna Otmianowska-Mazur","submitted_at":"2012-03-13T23:07:10Z","abstract_excerpt":"We study a model of fast magnetic reconnection in the presence of weak turbulence proposed by Lazarian and Vishniac (1999) using three-dimensional direct numerical simulations. The model has been already successfully tested in Kowal et al. (2009) confirming the dependencies of the reconnection speed $V_{rec}$ on the turbulence injection power $P_{inj}$ and the injection scale $l_{inj}$ expressed by a constraint $V_{rec} \\sim P_{inj}^{1/2} l_{inj}^{3/4}$ and no observed dependency on Ohmic resistivity. In Kowal et al. (2009), in order to drive turbulence, we injected velocity fluctuations in Fo"},"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":"1203.2971","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.SR","submitted_at":"2012-03-13T23:07:10Z","cross_cats_sorted":["physics.plasm-ph"],"title_canon_sha256":"3421441cc557f837ae13a78c5b1af24bf1fc28888c7ecb0c8000eeecb3578b19","abstract_canon_sha256":"c2c26c2905705cc163b6f8759b2532cad1b2c4f6f626e9be6905e6a67c9365b3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:58:09.070107Z","signature_b64":"VY6b7FQAaHIU3dhiYjZMq7q/O4peWcl+VI3CDOwn8lIU65snnnA4yfWIu3EZUwu1OOyGVWpdFMGbqmNZGFSnCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f69a44d8e545215cec9c6624ec960b2f80e6a34f2d8d82ee31c990eab934193b","last_reissued_at":"2026-05-18T01:58:09.069623Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:58:09.069623Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Reconnection Studies Under Different Types of Turbulence Driving","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.plasm-ph"],"primary_cat":"astro-ph.SR","authors_text":"Alex Lazarian, Ethan T. Vishniac, Grzegorz Kowal, Katarzyna Otmianowska-Mazur","submitted_at":"2012-03-13T23:07:10Z","abstract_excerpt":"We study a model of fast magnetic reconnection in the presence of weak turbulence proposed by Lazarian and Vishniac (1999) using three-dimensional direct numerical simulations. The model has been already successfully tested in Kowal et al. (2009) confirming the dependencies of the reconnection speed $V_{rec}$ on the turbulence injection power $P_{inj}$ and the injection scale $l_{inj}$ expressed by a constraint $V_{rec} \\sim P_{inj}^{1/2} l_{inj}^{3/4}$ and no observed dependency on Ohmic resistivity. In Kowal et al. (2009), in order to drive turbulence, we injected velocity fluctuations in Fo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1203.2971","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":"1203.2971","created_at":"2026-05-18T01:58:09.069704+00:00"},{"alias_kind":"arxiv_version","alias_value":"1203.2971v1","created_at":"2026-05-18T01:58:09.069704+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1203.2971","created_at":"2026-05-18T01:58:09.069704+00:00"},{"alias_kind":"pith_short_12","alias_value":"62NEJWHFIUQV","created_at":"2026-05-18T12:26:56.085431+00:00"},{"alias_kind":"pith_short_16","alias_value":"62NEJWHFIUQVZ3E4","created_at":"2026-05-18T12:26:56.085431+00:00"},{"alias_kind":"pith_short_8","alias_value":"62NEJWHF","created_at":"2026-05-18T12:26:56.085431+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.18946","citing_title":"Magnetic Prandtl number dependence of plasmoid-mediated reconnection","ref_index":18,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/62NEJWHFIUQVZ3E4MYSOZFQLF6","json":"https://pith.science/pith/62NEJWHFIUQVZ3E4MYSOZFQLF6.json","graph_json":"https://pith.science/api/pith-number/62NEJWHFIUQVZ3E4MYSOZFQLF6/graph.json","events_json":"https://pith.science/api/pith-number/62NEJWHFIUQVZ3E4MYSOZFQLF6/events.json","paper":"https://pith.science/paper/62NEJWHF"},"agent_actions":{"view_html":"https://pith.science/pith/62NEJWHFIUQVZ3E4MYSOZFQLF6","download_json":"https://pith.science/pith/62NEJWHFIUQVZ3E4MYSOZFQLF6.json","view_paper":"https://pith.science/paper/62NEJWHF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1203.2971&json=true","fetch_graph":"https://pith.science/api/pith-number/62NEJWHFIUQVZ3E4MYSOZFQLF6/graph.json","fetch_events":"https://pith.science/api/pith-number/62NEJWHFIUQVZ3E4MYSOZFQLF6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/62NEJWHFIUQVZ3E4MYSOZFQLF6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/62NEJWHFIUQVZ3E4MYSOZFQLF6/action/storage_attestation","attest_author":"https://pith.science/pith/62NEJWHFIUQVZ3E4MYSOZFQLF6/action/author_attestation","sign_citation":"https://pith.science/pith/62NEJWHFIUQVZ3E4MYSOZFQLF6/action/citation_signature","submit_replication":"https://pith.science/pith/62NEJWHFIUQVZ3E4MYSOZFQLF6/action/replication_record"}},"created_at":"2026-05-18T01:58:09.069704+00:00","updated_at":"2026-05-18T01:58:09.069704+00:00"}