{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:LCRBV3N52WORFLSQCLQWXB76V5","short_pith_number":"pith:LCRBV3N5","canonical_record":{"source":{"id":"1604.05300","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2016-04-17T15:20:36Z","cross_cats_sorted":[],"title_canon_sha256":"01c3a527e416e5f095f4fcd9f1f278e83d883ceb3166906b431a43941cffca3b","abstract_canon_sha256":"3245c03373535da0b631823152c9f88f11af1a386667f26f04d8b6e09720fcea"},"schema_version":"1.0"},"canonical_sha256":"58a21aedbdd59d12ae5012e16b87feaf5ac9b804bd4ca27c1fc1c7f93cd2c07f","source":{"kind":"arxiv","id":"1604.05300","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.05300","created_at":"2026-05-18T01:12:48Z"},{"alias_kind":"arxiv_version","alias_value":"1604.05300v2","created_at":"2026-05-18T01:12:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.05300","created_at":"2026-05-18T01:12:48Z"},{"alias_kind":"pith_short_12","alias_value":"LCRBV3N52WOR","created_at":"2026-05-18T12:30:29Z"},{"alias_kind":"pith_short_16","alias_value":"LCRBV3N52WORFLSQ","created_at":"2026-05-18T12:30:29Z"},{"alias_kind":"pith_short_8","alias_value":"LCRBV3N5","created_at":"2026-05-18T12:30:29Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:LCRBV3N52WORFLSQCLQWXB76V5","target":"record","payload":{"canonical_record":{"source":{"id":"1604.05300","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2016-04-17T15:20:36Z","cross_cats_sorted":[],"title_canon_sha256":"01c3a527e416e5f095f4fcd9f1f278e83d883ceb3166906b431a43941cffca3b","abstract_canon_sha256":"3245c03373535da0b631823152c9f88f11af1a386667f26f04d8b6e09720fcea"},"schema_version":"1.0"},"canonical_sha256":"58a21aedbdd59d12ae5012e16b87feaf5ac9b804bd4ca27c1fc1c7f93cd2c07f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:12:48.390845Z","signature_b64":"3+2ArRdyrXL3hgYylN52sxLhTLXQ1Y4uJ30Zb6kmsjT2kUZU0EemdOtFQx9fT097Bbzr03CPj7rriIbe/jAYAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"58a21aedbdd59d12ae5012e16b87feaf5ac9b804bd4ca27c1fc1c7f93cd2c07f","last_reissued_at":"2026-05-18T01:12:48.390461Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:12:48.390461Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1604.05300","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":"2026-05-18T01:12:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dMpJHpljfF3kRGyX3kILG29xlTTBa3WXEv2EaKcbZIjVVFUeX1yI3Yy3hsnhU0mZlMhW9FHWEpCH2ZcPVNN2Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T21:47:49.932462Z"},"content_sha256":"bce55e7e612d23b203f522c2321e16478ef035130f4ad596d2410da1873578db","schema_version":"1.0","event_id":"sha256:bce55e7e612d23b203f522c2321e16478ef035130f4ad596d2410da1873578db"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:LCRBV3N52WORFLSQCLQWXB76V5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Thermodynamics of charged rotating dilaton black branes coupled to logarithmic nonlinear electrodynamics","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"A. Sheykhi, M. H. Dehghani, M. Kord Zangeneh","submitted_at":"2016-04-17T15:20:36Z","abstract_excerpt":"We construct a new class of charged rotating black brane solutions in the presence of logarithmic nonlinear electrodynamics with complete set of the rotation parameters in arbitrary dimensions. The topology of the horizon of these rotating black branes are flat, while, due to the presence of the dilaton field the asymptotic behaviour of them are neither flat nor (anti)-de Sitter [(A)dS]. We investigate the physical properties of the solutions. The mass and angular momentum of the spacetime are obtained by using the counterterm method inspired by AdS/CFT correspondence. We derive temperature, e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.05300","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":"2026-05-18T01:12:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NelRY3FCHgZRVryyf0Nl+1xiEGDYmCziCd8Ia0U3qm1rNAVqiXwg7TH9BcaQG/15bCw1DRhegOJq3S892DwXCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T21:47:49.932810Z"},"content_sha256":"8b856d8137ab5faa9233438c57b4d242dd0619d0613359d8e6801d49999f3f52","schema_version":"1.0","event_id":"sha256:8b856d8137ab5faa9233438c57b4d242dd0619d0613359d8e6801d49999f3f52"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LCRBV3N52WORFLSQCLQWXB76V5/bundle.json","state_url":"https://pith.science/pith/LCRBV3N52WORFLSQCLQWXB76V5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LCRBV3N52WORFLSQCLQWXB76V5/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":"2026-06-03T21:47:49Z","links":{"resolver":"https://pith.science/pith/LCRBV3N52WORFLSQCLQWXB76V5","bundle":"https://pith.science/pith/LCRBV3N52WORFLSQCLQWXB76V5/bundle.json","state":"https://pith.science/pith/LCRBV3N52WORFLSQCLQWXB76V5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LCRBV3N52WORFLSQCLQWXB76V5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:LCRBV3N52WORFLSQCLQWXB76V5","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":"3245c03373535da0b631823152c9f88f11af1a386667f26f04d8b6e09720fcea","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2016-04-17T15:20:36Z","title_canon_sha256":"01c3a527e416e5f095f4fcd9f1f278e83d883ceb3166906b431a43941cffca3b"},"schema_version":"1.0","source":{"id":"1604.05300","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.05300","created_at":"2026-05-18T01:12:48Z"},{"alias_kind":"arxiv_version","alias_value":"1604.05300v2","created_at":"2026-05-18T01:12:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.05300","created_at":"2026-05-18T01:12:48Z"},{"alias_kind":"pith_short_12","alias_value":"LCRBV3N52WOR","created_at":"2026-05-18T12:30:29Z"},{"alias_kind":"pith_short_16","alias_value":"LCRBV3N52WORFLSQ","created_at":"2026-05-18T12:30:29Z"},{"alias_kind":"pith_short_8","alias_value":"LCRBV3N5","created_at":"2026-05-18T12:30:29Z"}],"graph_snapshots":[{"event_id":"sha256:8b856d8137ab5faa9233438c57b4d242dd0619d0613359d8e6801d49999f3f52","target":"graph","created_at":"2026-05-18T01:12:48Z","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":"We construct a new class of charged rotating black brane solutions in the presence of logarithmic nonlinear electrodynamics with complete set of the rotation parameters in arbitrary dimensions. The topology of the horizon of these rotating black branes are flat, while, due to the presence of the dilaton field the asymptotic behaviour of them are neither flat nor (anti)-de Sitter [(A)dS]. We investigate the physical properties of the solutions. The mass and angular momentum of the spacetime are obtained by using the counterterm method inspired by AdS/CFT correspondence. We derive temperature, e","authors_text":"A. Sheykhi, M. H. Dehghani, M. Kord Zangeneh","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2016-04-17T15:20:36Z","title":"Thermodynamics of charged rotating dilaton black branes coupled to logarithmic nonlinear electrodynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.05300","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:bce55e7e612d23b203f522c2321e16478ef035130f4ad596d2410da1873578db","target":"record","created_at":"2026-05-18T01:12:48Z","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":"3245c03373535da0b631823152c9f88f11af1a386667f26f04d8b6e09720fcea","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2016-04-17T15:20:36Z","title_canon_sha256":"01c3a527e416e5f095f4fcd9f1f278e83d883ceb3166906b431a43941cffca3b"},"schema_version":"1.0","source":{"id":"1604.05300","kind":"arxiv","version":2}},"canonical_sha256":"58a21aedbdd59d12ae5012e16b87feaf5ac9b804bd4ca27c1fc1c7f93cd2c07f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"58a21aedbdd59d12ae5012e16b87feaf5ac9b804bd4ca27c1fc1c7f93cd2c07f","first_computed_at":"2026-05-18T01:12:48.390461Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:12:48.390461Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"3+2ArRdyrXL3hgYylN52sxLhTLXQ1Y4uJ30Zb6kmsjT2kUZU0EemdOtFQx9fT097Bbzr03CPj7rriIbe/jAYAA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:12:48.390845Z","signed_message":"canonical_sha256_bytes"},"source_id":"1604.05300","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:bce55e7e612d23b203f522c2321e16478ef035130f4ad596d2410da1873578db","sha256:8b856d8137ab5faa9233438c57b4d242dd0619d0613359d8e6801d49999f3f52"],"state_sha256":"63baf0de90b490022508ad32616a9db16b018418ca37a90ee34cd7c7c3757d76"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IiJioHvrO9ovBbpAp9ON5ZUb9TOvI/ucLPITx5N9EejKuUquT9gQX4BO94Bf8MocJOURmcmJJIoKNG3ZUSrvBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T21:47:49.934758Z","bundle_sha256":"6d4b2ee2e05d76eacfb3894a5dae457c0b15f56ae0d0631cbfe12c068a439ddc"}}