{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:XFZBAVI5ZQWMAHJUCSVQ4CPMY7","short_pith_number":"pith:XFZBAVI5","schema_version":"1.0","canonical_sha256":"b97210551dcc2cc01d3414ab0e09ecc7fbd160bcf3d9f3be0ef137848c860aea","source":{"kind":"arxiv","id":"1706.01776","version":1},"attestation_state":"computed","paper":{"title":"Temperature Anisotropy Relaxation of the One-Component Plasma","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Jerome Daligault, Scott D. Baalrud","submitted_at":"2017-06-06T14:06:09Z","abstract_excerpt":"The relaxation rate of a Maxwellian velocity distribution function that has an initially anisotropic temperature $(T_\\parallel \\neq T_\\perp)$ is an important physical process in space and laboratory plasmas. It is also a canonical example of an energy transport process that can be used to test theory. Here, this rate is evaluated using molecular dynamics simulations of the one-component plasma. Results are compared with the predictions of four kinetic theories; two treating the weakly coupled regime (1) the Landau equation, and (2) the Lenard-Balescu equation, and two that attempt to extend th"},"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":"1706.01776","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-06-06T14:06:09Z","cross_cats_sorted":[],"title_canon_sha256":"dd95b7bb356ec07e81b17958308be0d3af9539a6c4c05da90806a29bb36afadb","abstract_canon_sha256":"0810a7e512df2c3e2fd9bf40922bac0b55b3f8140cf1323ab1d9ae31007dc712"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:42:55.991819Z","signature_b64":"bvekNudIGC//A5uO+E6B3IBW6MDjTFmgy1+G7DFJ6JVy6mXtl3toTT0Md0jXAwwOlKVT/uEKHyo3U5UKFKPfCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b97210551dcc2cc01d3414ab0e09ecc7fbd160bcf3d9f3be0ef137848c860aea","last_reissued_at":"2026-05-18T00:42:55.991009Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:42:55.991009Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Temperature Anisotropy Relaxation of the One-Component Plasma","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Jerome Daligault, Scott D. Baalrud","submitted_at":"2017-06-06T14:06:09Z","abstract_excerpt":"The relaxation rate of a Maxwellian velocity distribution function that has an initially anisotropic temperature $(T_\\parallel \\neq T_\\perp)$ is an important physical process in space and laboratory plasmas. It is also a canonical example of an energy transport process that can be used to test theory. Here, this rate is evaluated using molecular dynamics simulations of the one-component plasma. Results are compared with the predictions of four kinetic theories; two treating the weakly coupled regime (1) the Landau equation, and (2) the Lenard-Balescu equation, and two that attempt to extend th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.01776","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":"1706.01776","created_at":"2026-05-18T00:42:55.991138+00:00"},{"alias_kind":"arxiv_version","alias_value":"1706.01776v1","created_at":"2026-05-18T00:42:55.991138+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.01776","created_at":"2026-05-18T00:42:55.991138+00:00"},{"alias_kind":"pith_short_12","alias_value":"XFZBAVI5ZQWM","created_at":"2026-05-18T12:31:53.515858+00:00"},{"alias_kind":"pith_short_16","alias_value":"XFZBAVI5ZQWMAHJU","created_at":"2026-05-18T12:31:53.515858+00:00"},{"alias_kind":"pith_short_8","alias_value":"XFZBAVI5","created_at":"2026-05-18T12:31:53.515858+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/XFZBAVI5ZQWMAHJUCSVQ4CPMY7","json":"https://pith.science/pith/XFZBAVI5ZQWMAHJUCSVQ4CPMY7.json","graph_json":"https://pith.science/api/pith-number/XFZBAVI5ZQWMAHJUCSVQ4CPMY7/graph.json","events_json":"https://pith.science/api/pith-number/XFZBAVI5ZQWMAHJUCSVQ4CPMY7/events.json","paper":"https://pith.science/paper/XFZBAVI5"},"agent_actions":{"view_html":"https://pith.science/pith/XFZBAVI5ZQWMAHJUCSVQ4CPMY7","download_json":"https://pith.science/pith/XFZBAVI5ZQWMAHJUCSVQ4CPMY7.json","view_paper":"https://pith.science/paper/XFZBAVI5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1706.01776&json=true","fetch_graph":"https://pith.science/api/pith-number/XFZBAVI5ZQWMAHJUCSVQ4CPMY7/graph.json","fetch_events":"https://pith.science/api/pith-number/XFZBAVI5ZQWMAHJUCSVQ4CPMY7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XFZBAVI5ZQWMAHJUCSVQ4CPMY7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XFZBAVI5ZQWMAHJUCSVQ4CPMY7/action/storage_attestation","attest_author":"https://pith.science/pith/XFZBAVI5ZQWMAHJUCSVQ4CPMY7/action/author_attestation","sign_citation":"https://pith.science/pith/XFZBAVI5ZQWMAHJUCSVQ4CPMY7/action/citation_signature","submit_replication":"https://pith.science/pith/XFZBAVI5ZQWMAHJUCSVQ4CPMY7/action/replication_record"}},"created_at":"2026-05-18T00:42:55.991138+00:00","updated_at":"2026-05-18T00:42:55.991138+00:00"}