{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:DZ7VC37XCXAMPDNCFZKXRVPVLG","short_pith_number":"pith:DZ7VC37X","schema_version":"1.0","canonical_sha256":"1e7f516ff715c0c78da22e5578d5f5599b58a6d2dbd62918e026aa1104b33779","source":{"kind":"arxiv","id":"1502.03283","version":3},"attestation_state":"computed","paper":{"title":"Nonlinear dynamics of the ion Weibel-filamentation instability: an analytical model for the evolution of the plasma and spectral properties","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.HE"],"primary_cat":"physics.plasm-ph","authors_text":"A. Debayle, C. Ruyer, G. Bonnaud, L. Gremillet","submitted_at":"2015-02-11T12:39:01Z","abstract_excerpt":"We present a predictive model of the nonlinear phase of the Weibel instability induced by two symmetric, counter-streaming ion beams in the non-relativistic regime. This self-consistent model combines the quasilinear kinetic theory of Davidson et al. [Phys. Fluids 15, 317 (1972)] with a simple description of current filament coalescence. It allows us to follow the evolution of the ion parameters up to a stage close to complete isotropization, and is thus of prime interest to understand the dynamics of collisionless shock formation. Its predictions are supported by 2-D and 3-D particle-in-cell "},"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":"1502.03283","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2015-02-11T12:39:01Z","cross_cats_sorted":["astro-ph.HE"],"title_canon_sha256":"60839971080a51384fc55cc59f57a652ef08e88c8d3ccec583029f0d87388bcd","abstract_canon_sha256":"c584dd2bb8dd5f5bffdf081f368120fd584a41fded70bbff9137a43fdbb1d36f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:19:27.610612Z","signature_b64":"kvbhJQSXeBlkIYf7UV5+xp/CyzaeNstELjTdePIoZ46EfqBRn7doEEouyzeql+cRQG6+X/nbggczADI2CVzVBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1e7f516ff715c0c78da22e5578d5f5599b58a6d2dbd62918e026aa1104b33779","last_reissued_at":"2026-05-18T02:19:27.609865Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:19:27.609865Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nonlinear dynamics of the ion Weibel-filamentation instability: an analytical model for the evolution of the plasma and spectral properties","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.HE"],"primary_cat":"physics.plasm-ph","authors_text":"A. Debayle, C. Ruyer, G. Bonnaud, L. Gremillet","submitted_at":"2015-02-11T12:39:01Z","abstract_excerpt":"We present a predictive model of the nonlinear phase of the Weibel instability induced by two symmetric, counter-streaming ion beams in the non-relativistic regime. This self-consistent model combines the quasilinear kinetic theory of Davidson et al. [Phys. Fluids 15, 317 (1972)] with a simple description of current filament coalescence. It allows us to follow the evolution of the ion parameters up to a stage close to complete isotropization, and is thus of prime interest to understand the dynamics of collisionless shock formation. Its predictions are supported by 2-D and 3-D particle-in-cell "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1502.03283","kind":"arxiv","version":3},"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":"1502.03283","created_at":"2026-05-18T02:19:27.609978+00:00"},{"alias_kind":"arxiv_version","alias_value":"1502.03283v3","created_at":"2026-05-18T02:19:27.609978+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1502.03283","created_at":"2026-05-18T02:19:27.609978+00:00"},{"alias_kind":"pith_short_12","alias_value":"DZ7VC37XCXAM","created_at":"2026-05-18T12:29:17.054201+00:00"},{"alias_kind":"pith_short_16","alias_value":"DZ7VC37XCXAMPDNC","created_at":"2026-05-18T12:29:17.054201+00:00"},{"alias_kind":"pith_short_8","alias_value":"DZ7VC37X","created_at":"2026-05-18T12:29:17.054201+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/DZ7VC37XCXAMPDNCFZKXRVPVLG","json":"https://pith.science/pith/DZ7VC37XCXAMPDNCFZKXRVPVLG.json","graph_json":"https://pith.science/api/pith-number/DZ7VC37XCXAMPDNCFZKXRVPVLG/graph.json","events_json":"https://pith.science/api/pith-number/DZ7VC37XCXAMPDNCFZKXRVPVLG/events.json","paper":"https://pith.science/paper/DZ7VC37X"},"agent_actions":{"view_html":"https://pith.science/pith/DZ7VC37XCXAMPDNCFZKXRVPVLG","download_json":"https://pith.science/pith/DZ7VC37XCXAMPDNCFZKXRVPVLG.json","view_paper":"https://pith.science/paper/DZ7VC37X","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1502.03283&json=true","fetch_graph":"https://pith.science/api/pith-number/DZ7VC37XCXAMPDNCFZKXRVPVLG/graph.json","fetch_events":"https://pith.science/api/pith-number/DZ7VC37XCXAMPDNCFZKXRVPVLG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DZ7VC37XCXAMPDNCFZKXRVPVLG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DZ7VC37XCXAMPDNCFZKXRVPVLG/action/storage_attestation","attest_author":"https://pith.science/pith/DZ7VC37XCXAMPDNCFZKXRVPVLG/action/author_attestation","sign_citation":"https://pith.science/pith/DZ7VC37XCXAMPDNCFZKXRVPVLG/action/citation_signature","submit_replication":"https://pith.science/pith/DZ7VC37XCXAMPDNCFZKXRVPVLG/action/replication_record"}},"created_at":"2026-05-18T02:19:27.609978+00:00","updated_at":"2026-05-18T02:19:27.609978+00:00"}