{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:5R7QYZX7ODMTIOKSE64RR6QMFQ","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"1954151cf9da89d0a5174159daa1c6f9961f2c1d649a5dd4c39736ea66ae7d52","cross_cats_sorted":["physics.gen-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2010-03-03T23:36:48Z","title_canon_sha256":"76077837f5c4e80a6426ed024876bb5c99d5dadd6bd2010db42b0495dbb014dc"},"schema_version":"1.0","source":{"id":"1003.0933","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1003.0933","created_at":"2026-05-18T02:08:46Z"},{"alias_kind":"arxiv_version","alias_value":"1003.0933v1","created_at":"2026-05-18T02:08:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1003.0933","created_at":"2026-05-18T02:08:46Z"},{"alias_kind":"pith_short_12","alias_value":"5R7QYZX7ODMT","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_16","alias_value":"5R7QYZX7ODMTIOKS","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_8","alias_value":"5R7QYZX7","created_at":"2026-05-18T12:26:04Z"}],"graph_snapshots":[{"event_id":"sha256:e1baf1e0fad791cb0ab0077f7145588158c4adfd98efc8fe254d9c6038039d81","target":"graph","created_at":"2026-05-18T02:08:46Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"The $e-e$, $e-i$, $i-i$ and charge-charge static structure factors are calculated for alkali and Be$^{2+}$ plasmas using the method described by Gregori et al. in \\cite{bibGreg2006}. The dynamic structure factors for alkali plasmas are calculated using the method of moments \\cite{bibAdam83}, \\cite{bibAdam93}. In both methods the screened Hellmann-Gurskii-Krasko potential, obtained on the basis of Bogolyubov's method, has been used taking into account not only the quantum-mechanical effects but also the ion structure \\cite{bib73}.\n  PACS: 52.27.Aj (Alkali and alkaline earth plasmas, Static and ","authors_text":"(2) Instituto Universitario de Matem\\'atica Pura y Aplicada, Berlin, Camino de Vera s/n, Germany, Humboldt Universitat zu Berlin, I. M. Tkachenko (2) ((1) Institut f\\\"ur Physik, Spain), S. P. Sadykova (1), Universidad Polit\\'ecnica de Valencia, Valencia, W. Ebeling (1)","cross_cats":["physics.gen-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2010-03-03T23:36:48Z","title":"Static and Dynamic Structure Factors with Account of the Ion Structure for High-temperature Alkali and Alkaline Earth Plasmas"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1003.0933","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:ede4bf6ae0e7f9eba27233750f6cecff391e780065a45461ac56895b73d4dfe2","target":"record","created_at":"2026-05-18T02:08:46Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"1954151cf9da89d0a5174159daa1c6f9961f2c1d649a5dd4c39736ea66ae7d52","cross_cats_sorted":["physics.gen-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2010-03-03T23:36:48Z","title_canon_sha256":"76077837f5c4e80a6426ed024876bb5c99d5dadd6bd2010db42b0495dbb014dc"},"schema_version":"1.0","source":{"id":"1003.0933","kind":"arxiv","version":1}},"canonical_sha256":"ec7f0c66ff70d934395227b918fa0c2c29129f86a4a9d2907947756a497c7959","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ec7f0c66ff70d934395227b918fa0c2c29129f86a4a9d2907947756a497c7959","first_computed_at":"2026-05-18T02:08:46.670687Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:08:46.670687Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"MOxBXdFqZ5M2PeAgGV73ww1PNmj5oTier9fac3BpkL7p91fLxV4HBso+lCXiiEK7KY0SBZR8ur2VwLJ2MSJLCw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:08:46.671189Z","signed_message":"canonical_sha256_bytes"},"source_id":"1003.0933","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ede4bf6ae0e7f9eba27233750f6cecff391e780065a45461ac56895b73d4dfe2","sha256:e1baf1e0fad791cb0ab0077f7145588158c4adfd98efc8fe254d9c6038039d81"],"state_sha256":"ae24260a58f58e865d61d015ba995ad006aecd1e65053d42209f0c4307038c07"}