{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2009:MOH2FOTLCUBYB5U5YVRTR3HUK5","short_pith_number":"pith:MOH2FOTL","canonical_record":{"source":{"id":"0904.0065","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2009-04-01T06:04:26Z","cross_cats_sorted":["astro-ph.CO","hep-ph","hep-th","math-ph","math.MP"],"title_canon_sha256":"95771290d322e70e23340d1b6d0c24877d78f3d5a4f8b56e3ec42fde4db76fe5","abstract_canon_sha256":"31a8888fb5eff04460b8f626ddc96acf0af3a256b4a96df6f92cedf88030ec25"},"schema_version":"1.0"},"canonical_sha256":"638fa2ba6b150380f69dc56338ecf4575a637361c015f5795dad69bbe2b4267a","source":{"kind":"arxiv","id":"0904.0065","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0904.0065","created_at":"2026-05-18T04:25:51Z"},{"alias_kind":"arxiv_version","alias_value":"0904.0065v2","created_at":"2026-05-18T04:25:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0904.0065","created_at":"2026-05-18T04:25:51Z"},{"alias_kind":"pith_short_12","alias_value":"MOH2FOTLCUBY","created_at":"2026-05-18T12:26:00Z"},{"alias_kind":"pith_short_16","alias_value":"MOH2FOTLCUBYB5U5","created_at":"2026-05-18T12:26:00Z"},{"alias_kind":"pith_short_8","alias_value":"MOH2FOTL","created_at":"2026-05-18T12:26:00Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2009:MOH2FOTLCUBYB5U5YVRTR3HUK5","target":"record","payload":{"canonical_record":{"source":{"id":"0904.0065","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2009-04-01T06:04:26Z","cross_cats_sorted":["astro-ph.CO","hep-ph","hep-th","math-ph","math.MP"],"title_canon_sha256":"95771290d322e70e23340d1b6d0c24877d78f3d5a4f8b56e3ec42fde4db76fe5","abstract_canon_sha256":"31a8888fb5eff04460b8f626ddc96acf0af3a256b4a96df6f92cedf88030ec25"},"schema_version":"1.0"},"canonical_sha256":"638fa2ba6b150380f69dc56338ecf4575a637361c015f5795dad69bbe2b4267a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:25:51.304496Z","signature_b64":"jmCCAMrkh0eYtBjU7Fy5/5+/92hg+obt04KeQaiKZbRiL/riDmcHTPGAAhcWsCJ1/rXrGQ28tkve3ZnzA/38CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"638fa2ba6b150380f69dc56338ecf4575a637361c015f5795dad69bbe2b4267a","last_reissued_at":"2026-05-18T04:25:51.303960Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:25:51.303960Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0904.0065","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:25:51Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pQAavJZXnxKF77tYkNFAyhbQuRo0Du0PN+m+87TCEDBp/ItPJ3/9fSuIjEKqVYlOU1KUjLbIvOmhthsDYq+vCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T22:29:03.582824Z"},"content_sha256":"cdd2746268521ffe1d2624cc850648cd50e4523308deba28b17dba01be6d915b","schema_version":"1.0","event_id":"sha256:cdd2746268521ffe1d2624cc850648cd50e4523308deba28b17dba01be6d915b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2009:MOH2FOTLCUBYB5U5YVRTR3HUK5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"N-dimensional plane symmetric solution with perfect fluid source","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-ph","hep-th","math-ph","math.MP"],"primary_cat":"gr-qc","authors_text":"Hongsheng Zhang, Hyerim Noh","submitted_at":"2009-04-01T06:04:26Z","abstract_excerpt":"A new class of plane symmetric solution sourced by a perfect fluid is found in our recent work. An n-dimensional ($n\\geq 4$) global plane symmetric solution of Einstein field equation generated by a perfect fluid source is investigated, which is the direct generalization of our previous 4-dimensional solution. One time-like Killing vector and $(n-2)(n-1)/2$ space-like Killing vectors, which span a Euclidean group $G_{(n-2)(n-1)/2}$, are permitted in this solution. The regions of the parameters constrained by weak, strong and dominant energy conditions for the source are studied. The boundary c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0904.0065","kind":"arxiv","version":2},"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":"2026-05-18T04:25:51Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"a2grqLSJBfuy8OPogqRnelRlwdv5sxw03AO7CoNelzpMLe4GUXqnC/n2hqfxJfbL4Xfu5JU2GxTbw523Y9QzCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T22:29:03.583322Z"},"content_sha256":"c71caf82138ce1b9c1124f0a276125e566a92b59afbc71d54205fda63530144e","schema_version":"1.0","event_id":"sha256:c71caf82138ce1b9c1124f0a276125e566a92b59afbc71d54205fda63530144e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MOH2FOTLCUBYB5U5YVRTR3HUK5/bundle.json","state_url":"https://pith.science/pith/MOH2FOTLCUBYB5U5YVRTR3HUK5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MOH2FOTLCUBYB5U5YVRTR3HUK5/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":"2026-05-28T22:29:03Z","links":{"resolver":"https://pith.science/pith/MOH2FOTLCUBYB5U5YVRTR3HUK5","bundle":"https://pith.science/pith/MOH2FOTLCUBYB5U5YVRTR3HUK5/bundle.json","state":"https://pith.science/pith/MOH2FOTLCUBYB5U5YVRTR3HUK5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MOH2FOTLCUBYB5U5YVRTR3HUK5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2009:MOH2FOTLCUBYB5U5YVRTR3HUK5","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":"31a8888fb5eff04460b8f626ddc96acf0af3a256b4a96df6f92cedf88030ec25","cross_cats_sorted":["astro-ph.CO","hep-ph","hep-th","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2009-04-01T06:04:26Z","title_canon_sha256":"95771290d322e70e23340d1b6d0c24877d78f3d5a4f8b56e3ec42fde4db76fe5"},"schema_version":"1.0","source":{"id":"0904.0065","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0904.0065","created_at":"2026-05-18T04:25:51Z"},{"alias_kind":"arxiv_version","alias_value":"0904.0065v2","created_at":"2026-05-18T04:25:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0904.0065","created_at":"2026-05-18T04:25:51Z"},{"alias_kind":"pith_short_12","alias_value":"MOH2FOTLCUBY","created_at":"2026-05-18T12:26:00Z"},{"alias_kind":"pith_short_16","alias_value":"MOH2FOTLCUBYB5U5","created_at":"2026-05-18T12:26:00Z"},{"alias_kind":"pith_short_8","alias_value":"MOH2FOTL","created_at":"2026-05-18T12:26:00Z"}],"graph_snapshots":[{"event_id":"sha256:c71caf82138ce1b9c1124f0a276125e566a92b59afbc71d54205fda63530144e","target":"graph","created_at":"2026-05-18T04:25:51Z","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":"A new class of plane symmetric solution sourced by a perfect fluid is found in our recent work. An n-dimensional ($n\\geq 4$) global plane symmetric solution of Einstein field equation generated by a perfect fluid source is investigated, which is the direct generalization of our previous 4-dimensional solution. One time-like Killing vector and $(n-2)(n-1)/2$ space-like Killing vectors, which span a Euclidean group $G_{(n-2)(n-1)/2}$, are permitted in this solution. The regions of the parameters constrained by weak, strong and dominant energy conditions for the source are studied. The boundary c","authors_text":"Hongsheng Zhang, Hyerim Noh","cross_cats":["astro-ph.CO","hep-ph","hep-th","math-ph","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2009-04-01T06:04:26Z","title":"N-dimensional plane symmetric solution with perfect fluid source"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0904.0065","kind":"arxiv","version":2},"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:cdd2746268521ffe1d2624cc850648cd50e4523308deba28b17dba01be6d915b","target":"record","created_at":"2026-05-18T04:25:51Z","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":"31a8888fb5eff04460b8f626ddc96acf0af3a256b4a96df6f92cedf88030ec25","cross_cats_sorted":["astro-ph.CO","hep-ph","hep-th","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2009-04-01T06:04:26Z","title_canon_sha256":"95771290d322e70e23340d1b6d0c24877d78f3d5a4f8b56e3ec42fde4db76fe5"},"schema_version":"1.0","source":{"id":"0904.0065","kind":"arxiv","version":2}},"canonical_sha256":"638fa2ba6b150380f69dc56338ecf4575a637361c015f5795dad69bbe2b4267a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"638fa2ba6b150380f69dc56338ecf4575a637361c015f5795dad69bbe2b4267a","first_computed_at":"2026-05-18T04:25:51.303960Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:25:51.303960Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"jmCCAMrkh0eYtBjU7Fy5/5+/92hg+obt04KeQaiKZbRiL/riDmcHTPGAAhcWsCJ1/rXrGQ28tkve3ZnzA/38CQ==","signature_status":"signed_v1","signed_at":"2026-05-18T04:25:51.304496Z","signed_message":"canonical_sha256_bytes"},"source_id":"0904.0065","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cdd2746268521ffe1d2624cc850648cd50e4523308deba28b17dba01be6d915b","sha256:c71caf82138ce1b9c1124f0a276125e566a92b59afbc71d54205fda63530144e"],"state_sha256":"b5d162bdbf55dc60786d7d764acc97308788d16f85921786953ae89409b44fef"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/2LknWcigC/Qs0up4azMIensNbN/eYfM+VT7cg9ycR/9nmTcEmZAJ6c9FbadLB/wi0/vofiJvtDzZ9u48ZxoCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T22:29:03.585780Z","bundle_sha256":"65a727ad937971439dfd30e2607f0b64d65d7bfe07f1c79b4059e678e497c834"}}