{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:Q55B6R5O2USTHC3GZ7CKXT65G3","short_pith_number":"pith:Q55B6R5O","canonical_record":{"source":{"id":"1807.00377","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2018-07-01T19:27:29Z","cross_cats_sorted":["hep-th","math-ph","math.MP"],"title_canon_sha256":"6c7ab55b916ced9142c7d3df367dc093ca89c312d7764d01fdf2fe992a87b523","abstract_canon_sha256":"28b6f9d9964e91932820bfb3607e58de7dee8010fa10b524ec734cc5a131610f"},"schema_version":"1.0"},"canonical_sha256":"877a1f47aed525338b66cfc4abcfdd36da15951b108ab14991d0adaada9104e4","source":{"kind":"arxiv","id":"1807.00377","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1807.00377","created_at":"2026-05-18T00:05:04Z"},{"alias_kind":"arxiv_version","alias_value":"1807.00377v1","created_at":"2026-05-18T00:05:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.00377","created_at":"2026-05-18T00:05:04Z"},{"alias_kind":"pith_short_12","alias_value":"Q55B6R5O2UST","created_at":"2026-05-18T12:32:46Z"},{"alias_kind":"pith_short_16","alias_value":"Q55B6R5O2USTHC3G","created_at":"2026-05-18T12:32:46Z"},{"alias_kind":"pith_short_8","alias_value":"Q55B6R5O","created_at":"2026-05-18T12:32:46Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:Q55B6R5O2USTHC3GZ7CKXT65G3","target":"record","payload":{"canonical_record":{"source":{"id":"1807.00377","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2018-07-01T19:27:29Z","cross_cats_sorted":["hep-th","math-ph","math.MP"],"title_canon_sha256":"6c7ab55b916ced9142c7d3df367dc093ca89c312d7764d01fdf2fe992a87b523","abstract_canon_sha256":"28b6f9d9964e91932820bfb3607e58de7dee8010fa10b524ec734cc5a131610f"},"schema_version":"1.0"},"canonical_sha256":"877a1f47aed525338b66cfc4abcfdd36da15951b108ab14991d0adaada9104e4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:05:04.726170Z","signature_b64":"TyklBOiYBS6QVOVXMOrOiJlTbkoeVwg1hYCYN5Z8rw+RP0/HZlIebFNcAVXDiKp2cZKuFaiivH0zJcypg4K4BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"877a1f47aed525338b66cfc4abcfdd36da15951b108ab14991d0adaada9104e4","last_reissued_at":"2026-05-18T00:05:04.725448Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:05:04.725448Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1807.00377","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":"2026-05-18T00:05:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"d0uTXU68c3t3GTBWgygI9gTYARWCst5QLBpkyPjtjzDcKbSaGMPFCyIVZ3ThOufliuotaac3mWRkcuf9iM7GDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T18:41:23.361783Z"},"content_sha256":"c0c3fa9f7d7a5a627fa250d083488880187fb31b9ab08f0b2eb81a574216f0fe","schema_version":"1.0","event_id":"sha256:c0c3fa9f7d7a5a627fa250d083488880187fb31b9ab08f0b2eb81a574216f0fe"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:Q55B6R5O2USTHC3GZ7CKXT65G3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Black branes in four-dimensional conformal equivalent theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","math-ph","math.MP"],"primary_cat":"gr-qc","authors_text":"Alex Giacomini, Andronikos Paliathanasis, N. Dimakis","submitted_at":"2018-07-01T19:27:29Z","abstract_excerpt":"The physical properties of static analytic solutions which describe black brane geometries are discussed. In particular we study the similarities and differences of analytic black brane/string solutions in the Einstein and Jordan frames. The comparison is made between vacuum power law $f(R)$ gravity solutions and their conformal equivalents in the Einstein frame. In our analysis we examine how the geometrical and physical properties of these analytic axisymmetric solutions - such as singularities, the temperature and the entropy - are affected as we pass from one frame to the other."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.00377","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":"2026-05-18T00:05:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"v3E8abGQTaHMr5L+TXBZ3Wv8uOen2WmNoaC58mKD2S3LoYzTY8g2uvizIcQIz+wQahUUCulWI2ZiiHVzzED3CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T18:41:23.362529Z"},"content_sha256":"457eb7ed928cf15cdb52b334b9be70b6e3c0a369e5b37a95dabe5cdbf527340a","schema_version":"1.0","event_id":"sha256:457eb7ed928cf15cdb52b334b9be70b6e3c0a369e5b37a95dabe5cdbf527340a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/Q55B6R5O2USTHC3GZ7CKXT65G3/bundle.json","state_url":"https://pith.science/pith/Q55B6R5O2USTHC3GZ7CKXT65G3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/Q55B6R5O2USTHC3GZ7CKXT65G3/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":"2026-06-08T18:41:23Z","links":{"resolver":"https://pith.science/pith/Q55B6R5O2USTHC3GZ7CKXT65G3","bundle":"https://pith.science/pith/Q55B6R5O2USTHC3GZ7CKXT65G3/bundle.json","state":"https://pith.science/pith/Q55B6R5O2USTHC3GZ7CKXT65G3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/Q55B6R5O2USTHC3GZ7CKXT65G3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:Q55B6R5O2USTHC3GZ7CKXT65G3","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":"28b6f9d9964e91932820bfb3607e58de7dee8010fa10b524ec734cc5a131610f","cross_cats_sorted":["hep-th","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2018-07-01T19:27:29Z","title_canon_sha256":"6c7ab55b916ced9142c7d3df367dc093ca89c312d7764d01fdf2fe992a87b523"},"schema_version":"1.0","source":{"id":"1807.00377","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1807.00377","created_at":"2026-05-18T00:05:04Z"},{"alias_kind":"arxiv_version","alias_value":"1807.00377v1","created_at":"2026-05-18T00:05:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.00377","created_at":"2026-05-18T00:05:04Z"},{"alias_kind":"pith_short_12","alias_value":"Q55B6R5O2UST","created_at":"2026-05-18T12:32:46Z"},{"alias_kind":"pith_short_16","alias_value":"Q55B6R5O2USTHC3G","created_at":"2026-05-18T12:32:46Z"},{"alias_kind":"pith_short_8","alias_value":"Q55B6R5O","created_at":"2026-05-18T12:32:46Z"}],"graph_snapshots":[{"event_id":"sha256:457eb7ed928cf15cdb52b334b9be70b6e3c0a369e5b37a95dabe5cdbf527340a","target":"graph","created_at":"2026-05-18T00:05:04Z","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":"The physical properties of static analytic solutions which describe black brane geometries are discussed. In particular we study the similarities and differences of analytic black brane/string solutions in the Einstein and Jordan frames. The comparison is made between vacuum power law $f(R)$ gravity solutions and their conformal equivalents in the Einstein frame. In our analysis we examine how the geometrical and physical properties of these analytic axisymmetric solutions - such as singularities, the temperature and the entropy - are affected as we pass from one frame to the other.","authors_text":"Alex Giacomini, Andronikos Paliathanasis, N. Dimakis","cross_cats":["hep-th","math-ph","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2018-07-01T19:27:29Z","title":"Black branes in four-dimensional conformal equivalent theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.00377","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:c0c3fa9f7d7a5a627fa250d083488880187fb31b9ab08f0b2eb81a574216f0fe","target":"record","created_at":"2026-05-18T00:05:04Z","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":"28b6f9d9964e91932820bfb3607e58de7dee8010fa10b524ec734cc5a131610f","cross_cats_sorted":["hep-th","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2018-07-01T19:27:29Z","title_canon_sha256":"6c7ab55b916ced9142c7d3df367dc093ca89c312d7764d01fdf2fe992a87b523"},"schema_version":"1.0","source":{"id":"1807.00377","kind":"arxiv","version":1}},"canonical_sha256":"877a1f47aed525338b66cfc4abcfdd36da15951b108ab14991d0adaada9104e4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"877a1f47aed525338b66cfc4abcfdd36da15951b108ab14991d0adaada9104e4","first_computed_at":"2026-05-18T00:05:04.725448Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:05:04.725448Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"TyklBOiYBS6QVOVXMOrOiJlTbkoeVwg1hYCYN5Z8rw+RP0/HZlIebFNcAVXDiKp2cZKuFaiivH0zJcypg4K4BQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:05:04.726170Z","signed_message":"canonical_sha256_bytes"},"source_id":"1807.00377","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c0c3fa9f7d7a5a627fa250d083488880187fb31b9ab08f0b2eb81a574216f0fe","sha256:457eb7ed928cf15cdb52b334b9be70b6e3c0a369e5b37a95dabe5cdbf527340a"],"state_sha256":"552b1b22e9c325c729c07e55fd2b2c061c5dc43a1805282264ecb37c104c50a7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rgKSfVSKhP0SGc1rh1K5wN/4VLfCyTdglqr7h4AdoGQ0sCYTBs1N0QnPqm6SqKOcjWbilYcrMrhwfLi0ZvjYCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-08T18:41:23.366425Z","bundle_sha256":"5fae5e0289cec9c01d72c83d66a0ec51601f46142739c63fc722659305edbc7b"}}