{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:HECJPRDPMMDWUBGHNPVU3ZV3OY","short_pith_number":"pith:HECJPRDP","canonical_record":{"source":{"id":"1005.1402","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.DG","submitted_at":"2010-05-09T14:41:13Z","cross_cats_sorted":[],"title_canon_sha256":"28b6d09914c76e37d888651eb9db5af3ab307481d8ee9d7fcea1714b33e72c94","abstract_canon_sha256":"7858de0b781ddd31ed179e9a85dba8dd315c53e7d092b2a935283a0923dc2cea"},"schema_version":"1.0"},"canonical_sha256":"390497c46f63076a04c76beb4de6bb763aa4954fe64d0cdc4c586ce5b9b6d0d7","source":{"kind":"arxiv","id":"1005.1402","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1005.1402","created_at":"2026-05-18T04:31:41Z"},{"alias_kind":"arxiv_version","alias_value":"1005.1402v1","created_at":"2026-05-18T04:31:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1005.1402","created_at":"2026-05-18T04:31:41Z"},{"alias_kind":"pith_short_12","alias_value":"HECJPRDPMMDW","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_16","alias_value":"HECJPRDPMMDWUBGH","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_8","alias_value":"HECJPRDP","created_at":"2026-05-18T12:26:07Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:HECJPRDPMMDWUBGHNPVU3ZV3OY","target":"record","payload":{"canonical_record":{"source":{"id":"1005.1402","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.DG","submitted_at":"2010-05-09T14:41:13Z","cross_cats_sorted":[],"title_canon_sha256":"28b6d09914c76e37d888651eb9db5af3ab307481d8ee9d7fcea1714b33e72c94","abstract_canon_sha256":"7858de0b781ddd31ed179e9a85dba8dd315c53e7d092b2a935283a0923dc2cea"},"schema_version":"1.0"},"canonical_sha256":"390497c46f63076a04c76beb4de6bb763aa4954fe64d0cdc4c586ce5b9b6d0d7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:31:41.198459Z","signature_b64":"lrpyU/5xqr04gxHQ+Piph7VtZxMg24UJX6dl8ECMjoEbAt2SP+HSMI3ZZlCrTGDHkzxx7iZ7OwxVnVym3+/XBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"390497c46f63076a04c76beb4de6bb763aa4954fe64d0cdc4c586ce5b9b6d0d7","last_reissued_at":"2026-05-18T04:31:41.197853Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:31:41.197853Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1005.1402","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":"2026-05-18T04:31:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wr48HTG5jeIAFvrZYLk22LOU5r4LkTrjukUY1Yyzl8RnNORxAd2pW2H0jovG7+ignFvlPhGSFLyewnu7E3AeCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T01:43:13.950696Z"},"content_sha256":"7ffa1264233e59e01ec950edbbf2ff30710b9c7c5c469ace4a2c3d92100f9056","schema_version":"1.0","event_id":"sha256:7ffa1264233e59e01ec950edbbf2ff30710b9c7c5c469ace4a2c3d92100f9056"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:HECJPRDPMMDWUBGHNPVU3ZV3OY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Geometric Dynamics of Plasma in Jet Spaces with Berwald-Moor Metric","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"math.DG","authors_text":"Constantin Udriste, Mircea Neagu","submitted_at":"2010-05-09T14:41:13Z","abstract_excerpt":"In this paper we construct the differential equations of the stream lines that characterize plasma regarded as a non-isotropic medium geometrized by a jet rheonomic time-invariant Berwald-Moor metric. Section 1 contains historical notes regarding the Plasma Physics and its geometrical description. Section 2 analyzes the generalized Lagrange geometrical approach of the non-isotropic plasma on 1-jet spaces. Section 3 studies the non-isotropic plasma as a medium geometrized by the jet rheonomic Berwald-Moor metric."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1005.1402","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":"2026-05-18T04:31:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LVKpT7yEkVt5FamqXhNrtz9mHEZUT2QnmPGsSUHccpzHXF4QEKHsECdkz5X0MSa4rZvAUnaVnnqcdmC9g+k2Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T01:43:13.951028Z"},"content_sha256":"8fb1dd6284e4851665c9a0252f3397a876eec40eb0ba8a0984510233339c61cd","schema_version":"1.0","event_id":"sha256:8fb1dd6284e4851665c9a0252f3397a876eec40eb0ba8a0984510233339c61cd"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HECJPRDPMMDWUBGHNPVU3ZV3OY/bundle.json","state_url":"https://pith.science/pith/HECJPRDPMMDWUBGHNPVU3ZV3OY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HECJPRDPMMDWUBGHNPVU3ZV3OY/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":"2026-06-24T01:43:13Z","links":{"resolver":"https://pith.science/pith/HECJPRDPMMDWUBGHNPVU3ZV3OY","bundle":"https://pith.science/pith/HECJPRDPMMDWUBGHNPVU3ZV3OY/bundle.json","state":"https://pith.science/pith/HECJPRDPMMDWUBGHNPVU3ZV3OY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HECJPRDPMMDWUBGHNPVU3ZV3OY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:HECJPRDPMMDWUBGHNPVU3ZV3OY","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":"7858de0b781ddd31ed179e9a85dba8dd315c53e7d092b2a935283a0923dc2cea","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.DG","submitted_at":"2010-05-09T14:41:13Z","title_canon_sha256":"28b6d09914c76e37d888651eb9db5af3ab307481d8ee9d7fcea1714b33e72c94"},"schema_version":"1.0","source":{"id":"1005.1402","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1005.1402","created_at":"2026-05-18T04:31:41Z"},{"alias_kind":"arxiv_version","alias_value":"1005.1402v1","created_at":"2026-05-18T04:31:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1005.1402","created_at":"2026-05-18T04:31:41Z"},{"alias_kind":"pith_short_12","alias_value":"HECJPRDPMMDW","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_16","alias_value":"HECJPRDPMMDWUBGH","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_8","alias_value":"HECJPRDP","created_at":"2026-05-18T12:26:07Z"}],"graph_snapshots":[{"event_id":"sha256:8fb1dd6284e4851665c9a0252f3397a876eec40eb0ba8a0984510233339c61cd","target":"graph","created_at":"2026-05-18T04:31:41Z","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":"In this paper we construct the differential equations of the stream lines that characterize plasma regarded as a non-isotropic medium geometrized by a jet rheonomic time-invariant Berwald-Moor metric. Section 1 contains historical notes regarding the Plasma Physics and its geometrical description. Section 2 analyzes the generalized Lagrange geometrical approach of the non-isotropic plasma on 1-jet spaces. Section 3 studies the non-isotropic plasma as a medium geometrized by the jet rheonomic Berwald-Moor metric.","authors_text":"Constantin Udriste, Mircea Neagu","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.DG","submitted_at":"2010-05-09T14:41:13Z","title":"Geometric Dynamics of Plasma in Jet Spaces with Berwald-Moor Metric"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1005.1402","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":"sha256:7ffa1264233e59e01ec950edbbf2ff30710b9c7c5c469ace4a2c3d92100f9056","target":"record","created_at":"2026-05-18T04:31:41Z","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":"7858de0b781ddd31ed179e9a85dba8dd315c53e7d092b2a935283a0923dc2cea","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.DG","submitted_at":"2010-05-09T14:41:13Z","title_canon_sha256":"28b6d09914c76e37d888651eb9db5af3ab307481d8ee9d7fcea1714b33e72c94"},"schema_version":"1.0","source":{"id":"1005.1402","kind":"arxiv","version":1}},"canonical_sha256":"390497c46f63076a04c76beb4de6bb763aa4954fe64d0cdc4c586ce5b9b6d0d7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"390497c46f63076a04c76beb4de6bb763aa4954fe64d0cdc4c586ce5b9b6d0d7","first_computed_at":"2026-05-18T04:31:41.197853Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:31:41.197853Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"lrpyU/5xqr04gxHQ+Piph7VtZxMg24UJX6dl8ECMjoEbAt2SP+HSMI3ZZlCrTGDHkzxx7iZ7OwxVnVym3+/XBw==","signature_status":"signed_v1","signed_at":"2026-05-18T04:31:41.198459Z","signed_message":"canonical_sha256_bytes"},"source_id":"1005.1402","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7ffa1264233e59e01ec950edbbf2ff30710b9c7c5c469ace4a2c3d92100f9056","sha256:8fb1dd6284e4851665c9a0252f3397a876eec40eb0ba8a0984510233339c61cd"],"state_sha256":"bf9332ac3b44b150ea76c09eb9146d13d94c2f615a35988c76ee9b40b35b1bfa"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SBaOVJC8lhMtqcQunzWj4+E842I7QXNzTbcrnN33vxQkdmePruZ8bcUU6QzLp01UOb8q64d4QuyIffhrHDmICQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-24T01:43:13.952992Z","bundle_sha256":"1d7190e3a250c5696ac85e0d365ddcf4f031ba146fc41c714b7a4d26bbc802c1"}}