{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:MHRTCJSJL3ACFQ3WFXZMWIZZMJ","short_pith_number":"pith:MHRTCJSJ","schema_version":"1.0","canonical_sha256":"61e33126495ec022c3762df2cb233962565d087005d8aaf91829577897c91531","source":{"kind":"arxiv","id":"1502.07890","version":1},"attestation_state":"computed","paper":{"title":"From Vlasov-Poisson and Vlasov-Poisson-Fokker-Planck Systems to Incompressible Euler Equations: the case with finite charge","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"math.AP","authors_text":"David Chiron, Julien Barr\\'e, Nader Masmoudi, Thierry Goudon","submitted_at":"2015-02-27T13:33:32Z","abstract_excerpt":"We study the asymptotic regime of strong electric fields that leads from the Vlasov-Poisson system to the Incompressible Euler equations. We also deal with the Vlasov-Poisson-Fokker-Planck system which induces dissipative effects. The originality consists in considering a situation with a finite total charge confined by a strong external field. In turn, the limiting equation is set in a bounded domain, the shape of which is determined by the external confining potential. The analysis extends to the situation where the limiting density is non-homogeneous and where the Euler equation is replaced"},"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":"1502.07890","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.AP","submitted_at":"2015-02-27T13:33:32Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"ddd7b8f0bfa701c9b6c5f7a879ad165f5c28b7f6eb4b0d07d79ed05f99bdfc70","abstract_canon_sha256":"6efb42031b06ffbcb6fd20fd3fa0f98e1ee3ad8de27bfffe74447ccd2a059b05"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:26:01.920770Z","signature_b64":"UZmIpvpNG2zN9JgQhnyAC0UZA9RcNC2N08fCFxfDFXLRUN8xZvHYgLgh7behwDWbjaa1jduL0fKThr8cwPliDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"61e33126495ec022c3762df2cb233962565d087005d8aaf91829577897c91531","last_reissued_at":"2026-05-18T02:26:01.920307Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:26:01.920307Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"From Vlasov-Poisson and Vlasov-Poisson-Fokker-Planck Systems to Incompressible Euler Equations: the case with finite charge","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"math.AP","authors_text":"David Chiron, Julien Barr\\'e, Nader Masmoudi, Thierry Goudon","submitted_at":"2015-02-27T13:33:32Z","abstract_excerpt":"We study the asymptotic regime of strong electric fields that leads from the Vlasov-Poisson system to the Incompressible Euler equations. We also deal with the Vlasov-Poisson-Fokker-Planck system which induces dissipative effects. The originality consists in considering a situation with a finite total charge confined by a strong external field. In turn, the limiting equation is set in a bounded domain, the shape of which is determined by the external confining potential. The analysis extends to the situation where the limiting density is non-homogeneous and where the Euler equation is replaced"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1502.07890","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":"1502.07890","created_at":"2026-05-18T02:26:01.920394+00:00"},{"alias_kind":"arxiv_version","alias_value":"1502.07890v1","created_at":"2026-05-18T02:26:01.920394+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1502.07890","created_at":"2026-05-18T02:26:01.920394+00:00"},{"alias_kind":"pith_short_12","alias_value":"MHRTCJSJL3AC","created_at":"2026-05-18T12:29:32.376354+00:00"},{"alias_kind":"pith_short_16","alias_value":"MHRTCJSJL3ACFQ3W","created_at":"2026-05-18T12:29:32.376354+00:00"},{"alias_kind":"pith_short_8","alias_value":"MHRTCJSJ","created_at":"2026-05-18T12:29:32.376354+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/MHRTCJSJL3ACFQ3WFXZMWIZZMJ","json":"https://pith.science/pith/MHRTCJSJL3ACFQ3WFXZMWIZZMJ.json","graph_json":"https://pith.science/api/pith-number/MHRTCJSJL3ACFQ3WFXZMWIZZMJ/graph.json","events_json":"https://pith.science/api/pith-number/MHRTCJSJL3ACFQ3WFXZMWIZZMJ/events.json","paper":"https://pith.science/paper/MHRTCJSJ"},"agent_actions":{"view_html":"https://pith.science/pith/MHRTCJSJL3ACFQ3WFXZMWIZZMJ","download_json":"https://pith.science/pith/MHRTCJSJL3ACFQ3WFXZMWIZZMJ.json","view_paper":"https://pith.science/paper/MHRTCJSJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1502.07890&json=true","fetch_graph":"https://pith.science/api/pith-number/MHRTCJSJL3ACFQ3WFXZMWIZZMJ/graph.json","fetch_events":"https://pith.science/api/pith-number/MHRTCJSJL3ACFQ3WFXZMWIZZMJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MHRTCJSJL3ACFQ3WFXZMWIZZMJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MHRTCJSJL3ACFQ3WFXZMWIZZMJ/action/storage_attestation","attest_author":"https://pith.science/pith/MHRTCJSJL3ACFQ3WFXZMWIZZMJ/action/author_attestation","sign_citation":"https://pith.science/pith/MHRTCJSJL3ACFQ3WFXZMWIZZMJ/action/citation_signature","submit_replication":"https://pith.science/pith/MHRTCJSJL3ACFQ3WFXZMWIZZMJ/action/replication_record"}},"created_at":"2026-05-18T02:26:01.920394+00:00","updated_at":"2026-05-18T02:26:01.920394+00:00"}