{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2003:A7WWFVGIVA6Q5BDYWGNA5QVFWR","short_pith_number":"pith:A7WWFVGI","canonical_record":{"source":{"id":"hep-th/0312030","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2003-12-02T15:13:41Z","cross_cats_sorted":[],"title_canon_sha256":"5a2993536d87e9a6a1c270b4603ba82e8deaa840765cb765d0cd8474ab36b674","abstract_canon_sha256":"943afa909502a27fe777bfe656d66d8678fe53c3a59c998bcf97b0c3aae17be8"},"schema_version":"1.0"},"canonical_sha256":"07ed62d4c8a83d0e8478b19a0ec2a5b443f551dc91ceeddf6e70490f8ae6f911","source":{"kind":"arxiv","id":"hep-th/0312030","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0312030","created_at":"2026-07-04T16:41:29Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0312030v2","created_at":"2026-07-04T16:41:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0312030","created_at":"2026-07-04T16:41:29Z"},{"alias_kind":"pith_short_12","alias_value":"A7WWFVGIVA6Q","created_at":"2026-07-04T16:41:29Z"},{"alias_kind":"pith_short_16","alias_value":"A7WWFVGIVA6Q5BDY","created_at":"2026-07-04T16:41:29Z"},{"alias_kind":"pith_short_8","alias_value":"A7WWFVGI","created_at":"2026-07-04T16:41:29Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2003:A7WWFVGIVA6Q5BDYWGNA5QVFWR","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/0312030","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2003-12-02T15:13:41Z","cross_cats_sorted":[],"title_canon_sha256":"5a2993536d87e9a6a1c270b4603ba82e8deaa840765cb765d0cd8474ab36b674","abstract_canon_sha256":"943afa909502a27fe777bfe656d66d8678fe53c3a59c998bcf97b0c3aae17be8"},"schema_version":"1.0"},"canonical_sha256":"07ed62d4c8a83d0e8478b19a0ec2a5b443f551dc91ceeddf6e70490f8ae6f911","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:41:29.047885Z","signature_b64":"gL+wNuky/nxio6v8KcyQ+sfSdTnvGIVSl6r+jgU9C2PQzIITySyeXXUWPi5jzaCuKXGP7lQaacfFFpRiiAaTAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"07ed62d4c8a83d0e8478b19a0ec2a5b443f551dc91ceeddf6e70490f8ae6f911","last_reissued_at":"2026-07-04T16:41:29.047515Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:41:29.047515Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/0312030","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":"2026-07-04T16:41:29Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SWZwamZ2n9jurO5fq7U+1S6hq1yVOW5v60++L7C6Kn5Gnlgru8upxLnf0J+DPEHJabBq8/E6g7n7OSruqbU4BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-18T11:55:36.020412Z"},"content_sha256":"10c30c83f839b1028f4865669c1d1be52e356cb2d02f84f5d73e70087087a6d0","schema_version":"1.0","event_id":"sha256:10c30c83f839b1028f4865669c1d1be52e356cb2d02f84f5d73e70087087a6d0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2003:A7WWFVGIVA6Q5BDYWGNA5QVFWR","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Magnetic Branes in Gauss-Bonnet Gravity","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"M. H. Dehghani","submitted_at":"2003-12-02T15:13:41Z","abstract_excerpt":"We present two new classes of magnetic brane solutions in Einstein-Maxwell-Gauss-Bonnet gravity with a negative cosmological constant. The first class of solutions yields an $(n+1)$-dimensional spacetime with a longitudinal magnetic field generated by a static magnetic brane. We also generalize this solution to the case of spinning magnetic branes with one or more rotation parameters. We find that these solutions have no curvature singularity and no horizons, but have a conic geometry. In these spacetimes, when all the rotation parameters are zero, the electric field vanishes, and therefore th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0312030","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/0312030/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-04T16:41:29Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jPsBu0gwkK0QB3pm8XjiHJ/gGxobD+Bu4SQZHjbov/1++8QUgMlMZ9+AcVPtV2LLqAcXmqxu7jphY6mKrtEhAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-18T11:55:36.020901Z"},"content_sha256":"b4201cb3d6f611d1085626decee4795051384b39598e6221bc253a7ba3a37473","schema_version":"1.0","event_id":"sha256:b4201cb3d6f611d1085626decee4795051384b39598e6221bc253a7ba3a37473"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/A7WWFVGIVA6Q5BDYWGNA5QVFWR/bundle.json","state_url":"https://pith.science/pith/A7WWFVGIVA6Q5BDYWGNA5QVFWR/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/A7WWFVGIVA6Q5BDYWGNA5QVFWR/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":"2026-08-18T11:55:36Z","links":{"resolver":"https://pith.science/pith/A7WWFVGIVA6Q5BDYWGNA5QVFWR","bundle":"https://pith.science/pith/A7WWFVGIVA6Q5BDYWGNA5QVFWR/bundle.json","state":"https://pith.science/pith/A7WWFVGIVA6Q5BDYWGNA5QVFWR/state.json","well_known_bundle":"https://pith.science/.well-known/pith/A7WWFVGIVA6Q5BDYWGNA5QVFWR/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2003:A7WWFVGIVA6Q5BDYWGNA5QVFWR","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":"943afa909502a27fe777bfe656d66d8678fe53c3a59c998bcf97b0c3aae17be8","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"2003-12-02T15:13:41Z","title_canon_sha256":"5a2993536d87e9a6a1c270b4603ba82e8deaa840765cb765d0cd8474ab36b674"},"schema_version":"1.0","source":{"id":"hep-th/0312030","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0312030","created_at":"2026-07-04T16:41:29Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0312030v2","created_at":"2026-07-04T16:41:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0312030","created_at":"2026-07-04T16:41:29Z"},{"alias_kind":"pith_short_12","alias_value":"A7WWFVGIVA6Q","created_at":"2026-07-04T16:41:29Z"},{"alias_kind":"pith_short_16","alias_value":"A7WWFVGIVA6Q5BDY","created_at":"2026-07-04T16:41:29Z"},{"alias_kind":"pith_short_8","alias_value":"A7WWFVGI","created_at":"2026-07-04T16:41:29Z"}],"graph_snapshots":[{"event_id":"sha256:b4201cb3d6f611d1085626decee4795051384b39598e6221bc253a7ba3a37473","target":"graph","created_at":"2026-07-04T16:41:29Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-th/0312030/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present two new classes of magnetic brane solutions in Einstein-Maxwell-Gauss-Bonnet gravity with a negative cosmological constant. The first class of solutions yields an $(n+1)$-dimensional spacetime with a longitudinal magnetic field generated by a static magnetic brane. We also generalize this solution to the case of spinning magnetic branes with one or more rotation parameters. We find that these solutions have no curvature singularity and no horizons, but have a conic geometry. In these spacetimes, when all the rotation parameters are zero, the electric field vanishes, and therefore th","authors_text":"M. H. Dehghani","cross_cats":[],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"2003-12-02T15:13:41Z","title":"Magnetic Branes in Gauss-Bonnet Gravity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0312030","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":"sha256:10c30c83f839b1028f4865669c1d1be52e356cb2d02f84f5d73e70087087a6d0","target":"record","created_at":"2026-07-04T16:41:29Z","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":"943afa909502a27fe777bfe656d66d8678fe53c3a59c998bcf97b0c3aae17be8","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"2003-12-02T15:13:41Z","title_canon_sha256":"5a2993536d87e9a6a1c270b4603ba82e8deaa840765cb765d0cd8474ab36b674"},"schema_version":"1.0","source":{"id":"hep-th/0312030","kind":"arxiv","version":2}},"canonical_sha256":"07ed62d4c8a83d0e8478b19a0ec2a5b443f551dc91ceeddf6e70490f8ae6f911","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"07ed62d4c8a83d0e8478b19a0ec2a5b443f551dc91ceeddf6e70490f8ae6f911","first_computed_at":"2026-07-04T16:41:29.047515Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:41:29.047515Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"gL+wNuky/nxio6v8KcyQ+sfSdTnvGIVSl6r+jgU9C2PQzIITySyeXXUWPi5jzaCuKXGP7lQaacfFFpRiiAaTAQ==","signature_status":"signed_v1","signed_at":"2026-07-04T16:41:29.047885Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/0312030","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:10c30c83f839b1028f4865669c1d1be52e356cb2d02f84f5d73e70087087a6d0","sha256:b4201cb3d6f611d1085626decee4795051384b39598e6221bc253a7ba3a37473"],"state_sha256":"82647861465949ba80a7841ac90126aa6a5f56cf621afe9f12ad2ee541a68eb1"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/CslglA0OgDdqM72Gy/Tn3l6oVyB9DqPikQfEofM7JJmKslTLmwjAwYDFtvoNCqAq5Om3a8jKn4LEjyeIDU6Cw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-18T11:55:36.025171Z","bundle_sha256":"16850eeee68b9d24baa3ef2005b45088f9b92f6851539641555f78ef33b0f120"}}