{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:M7KM6ZQM53HLTWCIN4MSP3GEQX","short_pith_number":"pith:M7KM6ZQM","schema_version":"1.0","canonical_sha256":"67d4cf660ceeceb9d8486f1927ecc485f15b2ec44be08e5888756bc43d7b6c69","source":{"kind":"arxiv","id":"1906.08165","version":1},"attestation_state":"computed","paper":{"title":"Phase-space modelling of solid-state plasmas","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"Giovanni Manfredi, J\\'er\\^ome Hurst, Paul-Antoine Hervieux","submitted_at":"2019-06-19T15:43:07Z","abstract_excerpt":"Conduction electrons in metallic nano-objects ($\\rm 1\\,nm = 10^{-9}\\, m$) behave as mobile negative charges confined by a fixed positively-charged background, the atomic ions. In many respects, this electron gas displays typical plasma properties such as screening and Langmuir waves, with more or less pronounced quantum features depending on the size of the object. To study these dynamical effects, the mathematical artillery of condensed-matter theorists mainly relies on wave function $\\psi(r,t)$ based methods, such as the celebrated Hartree-Fock equations. The theoretical plasma physicist, 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":"1906.08165","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2019-06-19T15:43:07Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"a6394475569d4df830f758aaebdffe961f7a8ec900dc1f3521d4a9f1ccbc7d39","abstract_canon_sha256":"2fed80cb06f23058d138b02aac694e5d64d54a53dfa6dcbf9a78c29f1d01ac42"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:42:54.460475Z","signature_b64":"AJBOZEx0gX48ugFcoQ2eSgxY991KDyNvzXuWnMz+Cs9FLdjfI6GUCYxvjMgnDcRK1PGIGO50UAHczhDEAM78AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"67d4cf660ceeceb9d8486f1927ecc485f15b2ec44be08e5888756bc43d7b6c69","last_reissued_at":"2026-05-17T23:42:54.459771Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:42:54.459771Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phase-space modelling of solid-state plasmas","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"Giovanni Manfredi, J\\'er\\^ome Hurst, Paul-Antoine Hervieux","submitted_at":"2019-06-19T15:43:07Z","abstract_excerpt":"Conduction electrons in metallic nano-objects ($\\rm 1\\,nm = 10^{-9}\\, m$) behave as mobile negative charges confined by a fixed positively-charged background, the atomic ions. In many respects, this electron gas displays typical plasma properties such as screening and Langmuir waves, with more or less pronounced quantum features depending on the size of the object. To study these dynamical effects, the mathematical artillery of condensed-matter theorists mainly relies on wave function $\\psi(r,t)$ based methods, such as the celebrated Hartree-Fock equations. The theoretical plasma physicist, in"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1906.08165","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":"1906.08165","created_at":"2026-05-17T23:42:54.459915+00:00"},{"alias_kind":"arxiv_version","alias_value":"1906.08165v1","created_at":"2026-05-17T23:42:54.459915+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1906.08165","created_at":"2026-05-17T23:42:54.459915+00:00"},{"alias_kind":"pith_short_12","alias_value":"M7KM6ZQM53HL","created_at":"2026-05-18T12:33:21.387695+00:00"},{"alias_kind":"pith_short_16","alias_value":"M7KM6ZQM53HLTWCI","created_at":"2026-05-18T12:33:21.387695+00:00"},{"alias_kind":"pith_short_8","alias_value":"M7KM6ZQM","created_at":"2026-05-18T12:33:21.387695+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/M7KM6ZQM53HLTWCIN4MSP3GEQX","json":"https://pith.science/pith/M7KM6ZQM53HLTWCIN4MSP3GEQX.json","graph_json":"https://pith.science/api/pith-number/M7KM6ZQM53HLTWCIN4MSP3GEQX/graph.json","events_json":"https://pith.science/api/pith-number/M7KM6ZQM53HLTWCIN4MSP3GEQX/events.json","paper":"https://pith.science/paper/M7KM6ZQM"},"agent_actions":{"view_html":"https://pith.science/pith/M7KM6ZQM53HLTWCIN4MSP3GEQX","download_json":"https://pith.science/pith/M7KM6ZQM53HLTWCIN4MSP3GEQX.json","view_paper":"https://pith.science/paper/M7KM6ZQM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1906.08165&json=true","fetch_graph":"https://pith.science/api/pith-number/M7KM6ZQM53HLTWCIN4MSP3GEQX/graph.json","fetch_events":"https://pith.science/api/pith-number/M7KM6ZQM53HLTWCIN4MSP3GEQX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/M7KM6ZQM53HLTWCIN4MSP3GEQX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/M7KM6ZQM53HLTWCIN4MSP3GEQX/action/storage_attestation","attest_author":"https://pith.science/pith/M7KM6ZQM53HLTWCIN4MSP3GEQX/action/author_attestation","sign_citation":"https://pith.science/pith/M7KM6ZQM53HLTWCIN4MSP3GEQX/action/citation_signature","submit_replication":"https://pith.science/pith/M7KM6ZQM53HLTWCIN4MSP3GEQX/action/replication_record"}},"created_at":"2026-05-17T23:42:54.459915+00:00","updated_at":"2026-05-17T23:42:54.459915+00:00"}