{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2006:ARRJHPTKPFGRV5ZOBIXGPBJGKO","short_pith_number":"pith:ARRJHPTK","canonical_record":{"source":{"id":"astro-ph/0612332","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"astro-ph","submitted_at":"2006-12-13T01:28:09Z","cross_cats_sorted":[],"title_canon_sha256":"3592de1f3eb4adac2920b0e449384fa428f71b5176986a68a88384f8f6e17956","abstract_canon_sha256":"5ae4040054de19fe4407f8752b41da770330871f0fed39c7c5be9275661e7334"},"schema_version":"1.0"},"canonical_sha256":"046293be6a794d1af72e0a2e678526538cc6c0c572db6a205edcae082509449c","source":{"kind":"arxiv","id":"astro-ph/0612332","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"astro-ph/0612332","created_at":"2026-05-18T01:40:28Z"},{"alias_kind":"arxiv_version","alias_value":"astro-ph/0612332v1","created_at":"2026-05-18T01:40:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.astro-ph/0612332","created_at":"2026-05-18T01:40:28Z"},{"alias_kind":"pith_short_12","alias_value":"ARRJHPTKPFGR","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_16","alias_value":"ARRJHPTKPFGRV5ZO","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_8","alias_value":"ARRJHPTK","created_at":"2026-05-18T12:25:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2006:ARRJHPTKPFGRV5ZOBIXGPBJGKO","target":"record","payload":{"canonical_record":{"source":{"id":"astro-ph/0612332","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"astro-ph","submitted_at":"2006-12-13T01:28:09Z","cross_cats_sorted":[],"title_canon_sha256":"3592de1f3eb4adac2920b0e449384fa428f71b5176986a68a88384f8f6e17956","abstract_canon_sha256":"5ae4040054de19fe4407f8752b41da770330871f0fed39c7c5be9275661e7334"},"schema_version":"1.0"},"canonical_sha256":"046293be6a794d1af72e0a2e678526538cc6c0c572db6a205edcae082509449c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:40:28.470186Z","signature_b64":"PjrHMaaX6Tm8pyG9Q8MFpS6VUzxxYGa9OEaCQq3aTfgWKmh/FMMjxDSkCVb0j1ioMnc1dHAYO50cu5P0p2lSCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"046293be6a794d1af72e0a2e678526538cc6c0c572db6a205edcae082509449c","last_reissued_at":"2026-05-18T01:40:28.469601Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:40:28.469601Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"astro-ph/0612332","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":"2026-05-18T01:40:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JLvgKkBCqqRi4PjhhPHGowhlYytUHtMmC8JwOMW5YA4571BDJuLRBO/curw+W3dtVAggAegYyPJ5jt0mCSfvAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T21:38:09.846127Z"},"content_sha256":"dc2ddb637820acef694622e0a2e30c9834e5b05d8b356ac1d6d2014ea9ceae40","schema_version":"1.0","event_id":"sha256:dc2ddb637820acef694622e0a2e30c9834e5b05d8b356ac1d6d2014ea9ceae40"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2006:ARRJHPTKPFGRV5ZOBIXGPBJGKO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Thermoelectric and Thermomagnetic Effects in Dilute Plasmas","license":"","headline":"","cross_cats":[],"primary_cat":"astro-ph","authors_text":"A. L. Garcia-Perciante, A. Sandoval-Villalbazo, L. S. Garcia-Colin","submitted_at":"2006-12-13T01:28:09Z","abstract_excerpt":"When an electrically charged system is subjected to the action of an electromagnetic field, it responds by generating an electrical current. In the case of a multicomponent plasma other effects, the so called cross effects, influence the flow of charge as well as the heat flow. In this paper we discuss these effects and their corresponding transport coefficients in a fully ionized plasma using Boltzmann's equation. Applications to non-confined plasmas, specially to those prevailing in astrophysical systems are highlighted. Also, a detailed comparison is given with other available results."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"astro-ph/0612332","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":"2026-05-18T01:40:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"J2aM4B/LHhaguenRSblplm/pRX530Up5ofsgmEGthoNiWAr4roU0T7+5n5MpAX4zs5LhRz/DoZbeVlz1sR9iBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T21:38:09.846493Z"},"content_sha256":"1e79a27851d4d6eed6177525e0a006b3fbf0cdda0d83daf5884ff9464510d4a6","schema_version":"1.0","event_id":"sha256:1e79a27851d4d6eed6177525e0a006b3fbf0cdda0d83daf5884ff9464510d4a6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ARRJHPTKPFGRV5ZOBIXGPBJGKO/bundle.json","state_url":"https://pith.science/pith/ARRJHPTKPFGRV5ZOBIXGPBJGKO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ARRJHPTKPFGRV5ZOBIXGPBJGKO/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":"2026-06-24T21:38:09Z","links":{"resolver":"https://pith.science/pith/ARRJHPTKPFGRV5ZOBIXGPBJGKO","bundle":"https://pith.science/pith/ARRJHPTKPFGRV5ZOBIXGPBJGKO/bundle.json","state":"https://pith.science/pith/ARRJHPTKPFGRV5ZOBIXGPBJGKO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ARRJHPTKPFGRV5ZOBIXGPBJGKO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2006:ARRJHPTKPFGRV5ZOBIXGPBJGKO","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":"5ae4040054de19fe4407f8752b41da770330871f0fed39c7c5be9275661e7334","cross_cats_sorted":[],"license":"","primary_cat":"astro-ph","submitted_at":"2006-12-13T01:28:09Z","title_canon_sha256":"3592de1f3eb4adac2920b0e449384fa428f71b5176986a68a88384f8f6e17956"},"schema_version":"1.0","source":{"id":"astro-ph/0612332","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"astro-ph/0612332","created_at":"2026-05-18T01:40:28Z"},{"alias_kind":"arxiv_version","alias_value":"astro-ph/0612332v1","created_at":"2026-05-18T01:40:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.astro-ph/0612332","created_at":"2026-05-18T01:40:28Z"},{"alias_kind":"pith_short_12","alias_value":"ARRJHPTKPFGR","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_16","alias_value":"ARRJHPTKPFGRV5ZO","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_8","alias_value":"ARRJHPTK","created_at":"2026-05-18T12:25:53Z"}],"graph_snapshots":[{"event_id":"sha256:1e79a27851d4d6eed6177525e0a006b3fbf0cdda0d83daf5884ff9464510d4a6","target":"graph","created_at":"2026-05-18T01:40:28Z","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":"When an electrically charged system is subjected to the action of an electromagnetic field, it responds by generating an electrical current. In the case of a multicomponent plasma other effects, the so called cross effects, influence the flow of charge as well as the heat flow. In this paper we discuss these effects and their corresponding transport coefficients in a fully ionized plasma using Boltzmann's equation. Applications to non-confined plasmas, specially to those prevailing in astrophysical systems are highlighted. Also, a detailed comparison is given with other available results.","authors_text":"A. L. Garcia-Perciante, A. Sandoval-Villalbazo, L. S. Garcia-Colin","cross_cats":[],"headline":"","license":"","primary_cat":"astro-ph","submitted_at":"2006-12-13T01:28:09Z","title":"Thermoelectric and Thermomagnetic Effects in Dilute Plasmas"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"astro-ph/0612332","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:dc2ddb637820acef694622e0a2e30c9834e5b05d8b356ac1d6d2014ea9ceae40","target":"record","created_at":"2026-05-18T01:40:28Z","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":"5ae4040054de19fe4407f8752b41da770330871f0fed39c7c5be9275661e7334","cross_cats_sorted":[],"license":"","primary_cat":"astro-ph","submitted_at":"2006-12-13T01:28:09Z","title_canon_sha256":"3592de1f3eb4adac2920b0e449384fa428f71b5176986a68a88384f8f6e17956"},"schema_version":"1.0","source":{"id":"astro-ph/0612332","kind":"arxiv","version":1}},"canonical_sha256":"046293be6a794d1af72e0a2e678526538cc6c0c572db6a205edcae082509449c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"046293be6a794d1af72e0a2e678526538cc6c0c572db6a205edcae082509449c","first_computed_at":"2026-05-18T01:40:28.469601Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:40:28.469601Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"PjrHMaaX6Tm8pyG9Q8MFpS6VUzxxYGa9OEaCQq3aTfgWKmh/FMMjxDSkCVb0j1ioMnc1dHAYO50cu5P0p2lSCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:40:28.470186Z","signed_message":"canonical_sha256_bytes"},"source_id":"astro-ph/0612332","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:dc2ddb637820acef694622e0a2e30c9834e5b05d8b356ac1d6d2014ea9ceae40","sha256:1e79a27851d4d6eed6177525e0a006b3fbf0cdda0d83daf5884ff9464510d4a6"],"state_sha256":"f5e6bc1f1ae5f120c1866af2ff65c5f95c88c96cfed57831a024a435a3e91337"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"C3hF9qSpAVnhy/gQxiH6Z9Gp/gwwhrfI5GkBmz5lr1n8gFi/gouznWjb+nnPSTfbDB/EaOh62pIkBhAAzRdrCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-24T21:38:09.848405Z","bundle_sha256":"a4e33c95a6fa3216b693ea46057241ee6c2c0f30f8cde6ddc288ad4ac4fe971c"}}