{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:K2CITSJ2R7VHOGNS7HKYHRNOP4","short_pith_number":"pith:K2CITSJ2","schema_version":"1.0","canonical_sha256":"568489c93a8fea7719b2f9d583c5ae7f01a9b7652c4d5110d8029f358b11339e","source":{"kind":"arxiv","id":"1410.1206","version":1},"attestation_state":"computed","paper":{"title":"Electron Heating During Magnetic Reconnection: A Simulation Scaling Study","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.SR","physics.space-ph"],"primary_cat":"physics.plasm-ph","authors_text":"C. C. Haggerty, J. F. Drake, K. Malakit, M. A. Shay, M. Oieroset, M. Swisdak, P. A. Cassak, P. Wu, T. D. Phan","submitted_at":"2014-10-05T20:01:03Z","abstract_excerpt":"Electron bulk heating during magnetic reconnection with symmetric inflow conditions is examined using kinetic particle-in-cell (PIC) simulations. The degree of electron heating is well correlated with the inflowing Alfv\\'en speed $c_{Ar}$ based on the reconnecting magnetic field through the relation $\\Delta T_e = 0.033 \\,m_i\\,c_{Ar}^2$, where $\\Delta T_{e}$ is the increase in electron temperature. For the range of simulations performed, the heating shows almost no correlation with inflow total temperature $T_{tot} = T_i + T_e$ or plasma $\\beta$. An out-of-plane (guide) magnetic field of simila"},"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":"1410.1206","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2014-10-05T20:01:03Z","cross_cats_sorted":["astro-ph.SR","physics.space-ph"],"title_canon_sha256":"02bf87743e2fb7b255c11b190e87dc9c730fdb384d1ab91259a177bcb09c80dc","abstract_canon_sha256":"e4c3e2a38127316de98b51b8abb986784de941cae9545d10793872e7cbc37067"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:52.430480Z","signature_b64":"+Ev6iJaYDuOVXgVlPqYCYQmKtcau1+bScLagDNb2buJ7b4kaYMCC9pwTr7TJMV70/lO0VYinjrE1dZMC88fkDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"568489c93a8fea7719b2f9d583c5ae7f01a9b7652c4d5110d8029f358b11339e","last_reissued_at":"2026-05-18T01:41:52.429876Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:52.429876Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electron Heating During Magnetic Reconnection: A Simulation Scaling Study","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.SR","physics.space-ph"],"primary_cat":"physics.plasm-ph","authors_text":"C. C. Haggerty, J. F. Drake, K. Malakit, M. A. Shay, M. Oieroset, M. Swisdak, P. A. Cassak, P. Wu, T. D. Phan","submitted_at":"2014-10-05T20:01:03Z","abstract_excerpt":"Electron bulk heating during magnetic reconnection with symmetric inflow conditions is examined using kinetic particle-in-cell (PIC) simulations. The degree of electron heating is well correlated with the inflowing Alfv\\'en speed $c_{Ar}$ based on the reconnecting magnetic field through the relation $\\Delta T_e = 0.033 \\,m_i\\,c_{Ar}^2$, where $\\Delta T_{e}$ is the increase in electron temperature. For the range of simulations performed, the heating shows almost no correlation with inflow total temperature $T_{tot} = T_i + T_e$ or plasma $\\beta$. An out-of-plane (guide) magnetic field of simila"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.1206","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":"1410.1206","created_at":"2026-05-18T01:41:52.429974+00:00"},{"alias_kind":"arxiv_version","alias_value":"1410.1206v1","created_at":"2026-05-18T01:41:52.429974+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.1206","created_at":"2026-05-18T01:41:52.429974+00:00"},{"alias_kind":"pith_short_12","alias_value":"K2CITSJ2R7VH","created_at":"2026-05-18T12:28:35.611951+00:00"},{"alias_kind":"pith_short_16","alias_value":"K2CITSJ2R7VHOGNS","created_at":"2026-05-18T12:28:35.611951+00:00"},{"alias_kind":"pith_short_8","alias_value":"K2CITSJ2","created_at":"2026-05-18T12:28:35.611951+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/K2CITSJ2R7VHOGNS7HKYHRNOP4","json":"https://pith.science/pith/K2CITSJ2R7VHOGNS7HKYHRNOP4.json","graph_json":"https://pith.science/api/pith-number/K2CITSJ2R7VHOGNS7HKYHRNOP4/graph.json","events_json":"https://pith.science/api/pith-number/K2CITSJ2R7VHOGNS7HKYHRNOP4/events.json","paper":"https://pith.science/paper/K2CITSJ2"},"agent_actions":{"view_html":"https://pith.science/pith/K2CITSJ2R7VHOGNS7HKYHRNOP4","download_json":"https://pith.science/pith/K2CITSJ2R7VHOGNS7HKYHRNOP4.json","view_paper":"https://pith.science/paper/K2CITSJ2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1410.1206&json=true","fetch_graph":"https://pith.science/api/pith-number/K2CITSJ2R7VHOGNS7HKYHRNOP4/graph.json","fetch_events":"https://pith.science/api/pith-number/K2CITSJ2R7VHOGNS7HKYHRNOP4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/K2CITSJ2R7VHOGNS7HKYHRNOP4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/K2CITSJ2R7VHOGNS7HKYHRNOP4/action/storage_attestation","attest_author":"https://pith.science/pith/K2CITSJ2R7VHOGNS7HKYHRNOP4/action/author_attestation","sign_citation":"https://pith.science/pith/K2CITSJ2R7VHOGNS7HKYHRNOP4/action/citation_signature","submit_replication":"https://pith.science/pith/K2CITSJ2R7VHOGNS7HKYHRNOP4/action/replication_record"}},"created_at":"2026-05-18T01:41:52.429974+00:00","updated_at":"2026-05-18T01:41:52.429974+00:00"}