{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:5AHXAXNFR6D6G4KIMHMTMMM2BP","short_pith_number":"pith:5AHXAXNF","schema_version":"1.0","canonical_sha256":"e80f705da58f87e3714861d936319a0bde02cc32bf0580395e49ebe4d922392f","source":{"kind":"arxiv","id":"1208.2512","version":1},"attestation_state":"computed","paper":{"title":"The self-consistent determination of HF electroconductivity of strongly coupled plasmas","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"A. A. Mihajlov, Lj. M. Ignjatovic, V. A. Sreckovic, V. M. Adamyan","submitted_at":"2012-08-13T07:16:41Z","abstract_excerpt":"Here is presented the calculation of the dynamic electrical conductivity of fully ionized, strongly coupled plasmas as a function of the external electric field frequency $\\omega$. The calculations are based on the the formula for the energy-dependent collision frequency which is determined by means of the Green function theory methods, as a sum over the Matsubara frequencies. The domain of extremely high electron density: $10^{21}\\leq n_{e}\\leq 10^{24} \\textrm{cm}^{-3}$, and for the temperature varying from $10 \\textrm{kK}$ to $1.000 \\textrm{kK}$ was examined. The real and imaginary parts of "},"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":"1208.2512","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2012-08-13T07:16:41Z","cross_cats_sorted":[],"title_canon_sha256":"feb336a7aac50d01644cda687e7a941721443d1c31b51e2449bee0ba9d4cc67b","abstract_canon_sha256":"27e87d07559e17a679b869c27d17ea62a48b3ab7e90fd82a93b844f19e3b3c70"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:48:57.654844Z","signature_b64":"jhIjzf7nvBNbw9c8roRJLIaoObhxrWMIPUuA0ZNtQQJR8+KKM/didIGbdNS6tUxkYghuLp+i26GCynxLG3nZDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e80f705da58f87e3714861d936319a0bde02cc32bf0580395e49ebe4d922392f","last_reissued_at":"2026-05-18T03:48:57.654391Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:48:57.654391Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The self-consistent determination of HF electroconductivity of strongly coupled plasmas","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"A. A. Mihajlov, Lj. M. Ignjatovic, V. A. Sreckovic, V. M. Adamyan","submitted_at":"2012-08-13T07:16:41Z","abstract_excerpt":"Here is presented the calculation of the dynamic electrical conductivity of fully ionized, strongly coupled plasmas as a function of the external electric field frequency $\\omega$. The calculations are based on the the formula for the energy-dependent collision frequency which is determined by means of the Green function theory methods, as a sum over the Matsubara frequencies. The domain of extremely high electron density: $10^{21}\\leq n_{e}\\leq 10^{24} \\textrm{cm}^{-3}$, and for the temperature varying from $10 \\textrm{kK}$ to $1.000 \\textrm{kK}$ was examined. The real and imaginary parts of "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1208.2512","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":"1208.2512","created_at":"2026-05-18T03:48:57.654452+00:00"},{"alias_kind":"arxiv_version","alias_value":"1208.2512v1","created_at":"2026-05-18T03:48:57.654452+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1208.2512","created_at":"2026-05-18T03:48:57.654452+00:00"},{"alias_kind":"pith_short_12","alias_value":"5AHXAXNFR6D6","created_at":"2026-05-18T12:26:53.410803+00:00"},{"alias_kind":"pith_short_16","alias_value":"5AHXAXNFR6D6G4KI","created_at":"2026-05-18T12:26:53.410803+00:00"},{"alias_kind":"pith_short_8","alias_value":"5AHXAXNF","created_at":"2026-05-18T12:26:53.410803+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/5AHXAXNFR6D6G4KIMHMTMMM2BP","json":"https://pith.science/pith/5AHXAXNFR6D6G4KIMHMTMMM2BP.json","graph_json":"https://pith.science/api/pith-number/5AHXAXNFR6D6G4KIMHMTMMM2BP/graph.json","events_json":"https://pith.science/api/pith-number/5AHXAXNFR6D6G4KIMHMTMMM2BP/events.json","paper":"https://pith.science/paper/5AHXAXNF"},"agent_actions":{"view_html":"https://pith.science/pith/5AHXAXNFR6D6G4KIMHMTMMM2BP","download_json":"https://pith.science/pith/5AHXAXNFR6D6G4KIMHMTMMM2BP.json","view_paper":"https://pith.science/paper/5AHXAXNF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1208.2512&json=true","fetch_graph":"https://pith.science/api/pith-number/5AHXAXNFR6D6G4KIMHMTMMM2BP/graph.json","fetch_events":"https://pith.science/api/pith-number/5AHXAXNFR6D6G4KIMHMTMMM2BP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5AHXAXNFR6D6G4KIMHMTMMM2BP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5AHXAXNFR6D6G4KIMHMTMMM2BP/action/storage_attestation","attest_author":"https://pith.science/pith/5AHXAXNFR6D6G4KIMHMTMMM2BP/action/author_attestation","sign_citation":"https://pith.science/pith/5AHXAXNFR6D6G4KIMHMTMMM2BP/action/citation_signature","submit_replication":"https://pith.science/pith/5AHXAXNFR6D6G4KIMHMTMMM2BP/action/replication_record"}},"created_at":"2026-05-18T03:48:57.654452+00:00","updated_at":"2026-05-18T03:48:57.654452+00:00"}