{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:ZRKHPXLDCQUJ4BWO4NZD34C3II","short_pith_number":"pith:ZRKHPXLD","schema_version":"1.0","canonical_sha256":"cc5477dd6314289e06cee3723df05b423308f56a180027a39c2d41efb52ce963","source":{"kind":"arxiv","id":"1307.8147","version":1},"attestation_state":"computed","paper":{"title":"Wave dispersion derived from the square-root Klein-Gordon-Poisson system","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Fernando Haas","submitted_at":"2013-07-30T21:02:33Z","abstract_excerpt":"Recently there has been great interest around quantum relativistic models for plasmas. In particular striking advances have been obtained by means of the Klein-Gordon-Maxwell system, which provides a first order approach to the relativistic regimes of quantum plasmas. It is a reliable method as long as the plasma spin dynamics is not a fundamental aspect, to be addressed using more refined (and heavier) models involving the Pauli-Schr\\\"odinger or Dirac equations. In this work a further simplification is considered, tracing back to the early days of relativistic quantum theory. Namely, we revis"},"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":"1307.8147","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-07-30T21:02:33Z","cross_cats_sorted":[],"title_canon_sha256":"7039a67155a902ef6b2681357db617247a6ff6a6bcc6662fb9d63a0dfa84b02e","abstract_canon_sha256":"0df7198cff93528fa64fd123a2fdf967028cf8bbd299d8995e156dfe8e16247b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:48:32.529391Z","signature_b64":"jnHTlhkVLiL/zJm2fvR64pi3WMdNAG3e5wGRLFNWF+ImTqqhXlUaxs6/b28Fl3Hty2M4d2g7XIDKhXwd2JaoCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cc5477dd6314289e06cee3723df05b423308f56a180027a39c2d41efb52ce963","last_reissued_at":"2026-05-18T01:48:32.528856Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:48:32.528856Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Wave dispersion derived from the square-root Klein-Gordon-Poisson system","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Fernando Haas","submitted_at":"2013-07-30T21:02:33Z","abstract_excerpt":"Recently there has been great interest around quantum relativistic models for plasmas. In particular striking advances have been obtained by means of the Klein-Gordon-Maxwell system, which provides a first order approach to the relativistic regimes of quantum plasmas. It is a reliable method as long as the plasma spin dynamics is not a fundamental aspect, to be addressed using more refined (and heavier) models involving the Pauli-Schr\\\"odinger or Dirac equations. In this work a further simplification is considered, tracing back to the early days of relativistic quantum theory. Namely, we revis"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1307.8147","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":"1307.8147","created_at":"2026-05-18T01:48:32.528940+00:00"},{"alias_kind":"arxiv_version","alias_value":"1307.8147v1","created_at":"2026-05-18T01:48:32.528940+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1307.8147","created_at":"2026-05-18T01:48:32.528940+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZRKHPXLDCQUJ","created_at":"2026-05-18T12:28:09.283467+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZRKHPXLDCQUJ4BWO","created_at":"2026-05-18T12:28:09.283467+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZRKHPXLD","created_at":"2026-05-18T12:28:09.283467+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/ZRKHPXLDCQUJ4BWO4NZD34C3II","json":"https://pith.science/pith/ZRKHPXLDCQUJ4BWO4NZD34C3II.json","graph_json":"https://pith.science/api/pith-number/ZRKHPXLDCQUJ4BWO4NZD34C3II/graph.json","events_json":"https://pith.science/api/pith-number/ZRKHPXLDCQUJ4BWO4NZD34C3II/events.json","paper":"https://pith.science/paper/ZRKHPXLD"},"agent_actions":{"view_html":"https://pith.science/pith/ZRKHPXLDCQUJ4BWO4NZD34C3II","download_json":"https://pith.science/pith/ZRKHPXLDCQUJ4BWO4NZD34C3II.json","view_paper":"https://pith.science/paper/ZRKHPXLD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1307.8147&json=true","fetch_graph":"https://pith.science/api/pith-number/ZRKHPXLDCQUJ4BWO4NZD34C3II/graph.json","fetch_events":"https://pith.science/api/pith-number/ZRKHPXLDCQUJ4BWO4NZD34C3II/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZRKHPXLDCQUJ4BWO4NZD34C3II/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZRKHPXLDCQUJ4BWO4NZD34C3II/action/storage_attestation","attest_author":"https://pith.science/pith/ZRKHPXLDCQUJ4BWO4NZD34C3II/action/author_attestation","sign_citation":"https://pith.science/pith/ZRKHPXLDCQUJ4BWO4NZD34C3II/action/citation_signature","submit_replication":"https://pith.science/pith/ZRKHPXLDCQUJ4BWO4NZD34C3II/action/replication_record"}},"created_at":"2026-05-18T01:48:32.528940+00:00","updated_at":"2026-05-18T01:48:32.528940+00:00"}