{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:KDA6Z6AKC3GCVAKZTJLOQ6DHXO","short_pith_number":"pith:KDA6Z6AK","canonical_record":{"source":{"id":"1707.01509","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-07-05T18:01:43Z","cross_cats_sorted":[],"title_canon_sha256":"427904a45e3e309f118aff830791dc058ca3cab35e5155f4181c6496314a6a61","abstract_canon_sha256":"e0dc5175cd3e4f3b8b47918340676833f00b38cd9e88ae57d2177d5de3ac1553"},"schema_version":"1.0"},"canonical_sha256":"50c1ecf80a16cc2a81599a56e87867bb97f01da7ef1496e4c0a32ee2ba5cb243","source":{"kind":"arxiv","id":"1707.01509","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1707.01509","created_at":"2026-05-18T00:35:19Z"},{"alias_kind":"arxiv_version","alias_value":"1707.01509v1","created_at":"2026-05-18T00:35:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.01509","created_at":"2026-05-18T00:35:19Z"},{"alias_kind":"pith_short_12","alias_value":"KDA6Z6AKC3GC","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_16","alias_value":"KDA6Z6AKC3GCVAKZ","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_8","alias_value":"KDA6Z6AK","created_at":"2026-05-18T12:31:24Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:KDA6Z6AKC3GCVAKZTJLOQ6DHXO","target":"record","payload":{"canonical_record":{"source":{"id":"1707.01509","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-07-05T18:01:43Z","cross_cats_sorted":[],"title_canon_sha256":"427904a45e3e309f118aff830791dc058ca3cab35e5155f4181c6496314a6a61","abstract_canon_sha256":"e0dc5175cd3e4f3b8b47918340676833f00b38cd9e88ae57d2177d5de3ac1553"},"schema_version":"1.0"},"canonical_sha256":"50c1ecf80a16cc2a81599a56e87867bb97f01da7ef1496e4c0a32ee2ba5cb243","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:35:19.603327Z","signature_b64":"yiqBJ8+sXQ7/fKNwzDh1FJGA5NX+04Uf93RJ/ulu3y2aBOzhWqz7RIrnRsCe6/hjwxqrfrWnsBuIc9zISrFaBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"50c1ecf80a16cc2a81599a56e87867bb97f01da7ef1496e4c0a32ee2ba5cb243","last_reissued_at":"2026-05-18T00:35:19.602893Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:35:19.602893Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1707.01509","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:35:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zBCBPrx/TDLfF0cqdy1qTga7pi7ZmSpAuDrGG1jI98LQIECZwTNWspEW8253T3sByeYLPKApfJDbJzu0deWADw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T18:12:42.293307Z"},"content_sha256":"0ca56a06a52473c37305d1bc8859b8761745bbf108a756e7b06765a696de49ae","schema_version":"1.0","event_id":"sha256:0ca56a06a52473c37305d1bc8859b8761745bbf108a756e7b06765a696de49ae"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:KDA6Z6AKC3GCVAKZTJLOQ6DHXO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Pair Correlation Functions of Strongly Coupled Two-Temperature Plasma","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Nathaniel R. Shaffer, Sanat Kumar Tiwari, Scott D. Baalrud","submitted_at":"2017-07-05T18:01:43Z","abstract_excerpt":"Using molecular dynamics simulations, we perform the first direct tests of three proposed models for the pair correlation functions of strongly coupled plasmas with species of unequal temperature. The models are all extensions of the Ornstein-Zernike/hypernetted-chain theory used to good success for equilibrium plasmas. Each theory is evaluated at several coupling strengths, temperature ratios, and mass ratios for a model plasma in which the electrons are positively charged. We show that the model proposed by Seuferling, Vogel, and Teopffer [Phys. Rev. A 40, 323 (1989)] agrees well with molecu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.01509","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:35:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Wnnv4/pWf4Xq6F58HlTsFVHlFnQuex2Q0hK6qUD6Kg3ztbi6VF5BAhVX6+kIuBec2kypLUW83xCf/olepYmqBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T18:12:42.294117Z"},"content_sha256":"dca183253a921c3bd9cf40ca311d376e409ccbbf7d284ea2af19aa54444a9b58","schema_version":"1.0","event_id":"sha256:dca183253a921c3bd9cf40ca311d376e409ccbbf7d284ea2af19aa54444a9b58"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KDA6Z6AKC3GCVAKZTJLOQ6DHXO/bundle.json","state_url":"https://pith.science/pith/KDA6Z6AKC3GCVAKZTJLOQ6DHXO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KDA6Z6AKC3GCVAKZTJLOQ6DHXO/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-09T18:12:42Z","links":{"resolver":"https://pith.science/pith/KDA6Z6AKC3GCVAKZTJLOQ6DHXO","bundle":"https://pith.science/pith/KDA6Z6AKC3GCVAKZTJLOQ6DHXO/bundle.json","state":"https://pith.science/pith/KDA6Z6AKC3GCVAKZTJLOQ6DHXO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KDA6Z6AKC3GCVAKZTJLOQ6DHXO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:KDA6Z6AKC3GCVAKZTJLOQ6DHXO","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":"e0dc5175cd3e4f3b8b47918340676833f00b38cd9e88ae57d2177d5de3ac1553","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-07-05T18:01:43Z","title_canon_sha256":"427904a45e3e309f118aff830791dc058ca3cab35e5155f4181c6496314a6a61"},"schema_version":"1.0","source":{"id":"1707.01509","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1707.01509","created_at":"2026-05-18T00:35:19Z"},{"alias_kind":"arxiv_version","alias_value":"1707.01509v1","created_at":"2026-05-18T00:35:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.01509","created_at":"2026-05-18T00:35:19Z"},{"alias_kind":"pith_short_12","alias_value":"KDA6Z6AKC3GC","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_16","alias_value":"KDA6Z6AKC3GCVAKZ","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_8","alias_value":"KDA6Z6AK","created_at":"2026-05-18T12:31:24Z"}],"graph_snapshots":[{"event_id":"sha256:dca183253a921c3bd9cf40ca311d376e409ccbbf7d284ea2af19aa54444a9b58","target":"graph","created_at":"2026-05-18T00:35:19Z","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":"Using molecular dynamics simulations, we perform the first direct tests of three proposed models for the pair correlation functions of strongly coupled plasmas with species of unequal temperature. The models are all extensions of the Ornstein-Zernike/hypernetted-chain theory used to good success for equilibrium plasmas. Each theory is evaluated at several coupling strengths, temperature ratios, and mass ratios for a model plasma in which the electrons are positively charged. We show that the model proposed by Seuferling, Vogel, and Teopffer [Phys. Rev. A 40, 323 (1989)] agrees well with molecu","authors_text":"Nathaniel R. Shaffer, Sanat Kumar Tiwari, Scott D. Baalrud","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-07-05T18:01:43Z","title":"Pair Correlation Functions of Strongly Coupled Two-Temperature Plasma"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.01509","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":"sha256:0ca56a06a52473c37305d1bc8859b8761745bbf108a756e7b06765a696de49ae","target":"record","created_at":"2026-05-18T00:35:19Z","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":"e0dc5175cd3e4f3b8b47918340676833f00b38cd9e88ae57d2177d5de3ac1553","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-07-05T18:01:43Z","title_canon_sha256":"427904a45e3e309f118aff830791dc058ca3cab35e5155f4181c6496314a6a61"},"schema_version":"1.0","source":{"id":"1707.01509","kind":"arxiv","version":1}},"canonical_sha256":"50c1ecf80a16cc2a81599a56e87867bb97f01da7ef1496e4c0a32ee2ba5cb243","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"50c1ecf80a16cc2a81599a56e87867bb97f01da7ef1496e4c0a32ee2ba5cb243","first_computed_at":"2026-05-18T00:35:19.602893Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:35:19.602893Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"yiqBJ8+sXQ7/fKNwzDh1FJGA5NX+04Uf93RJ/ulu3y2aBOzhWqz7RIrnRsCe6/hjwxqrfrWnsBuIc9zISrFaBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:35:19.603327Z","signed_message":"canonical_sha256_bytes"},"source_id":"1707.01509","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0ca56a06a52473c37305d1bc8859b8761745bbf108a756e7b06765a696de49ae","sha256:dca183253a921c3bd9cf40ca311d376e409ccbbf7d284ea2af19aa54444a9b58"],"state_sha256":"09fd617f0b9d99d64852afa388d7014d0e96903f84d060c20bd48421c073ee34"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"neMvGiIPuijqN8JW/1XMcPBhRQgeFhQay6HtXXHEF9N8+FOEhtaEcDSySF5OwN1oohxOqEE8oumSTo/vZo0dDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T18:12:42.298494Z","bundle_sha256":"5bae6220dbe2641a27ad297afbf892376fc51c7284b370c4616e0046d14dd8eb"}}