{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:VFTD5GQDJBIPCAZXADM6NOMCOK","short_pith_number":"pith:VFTD5GQD","canonical_record":{"source":{"id":"1705.00862","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-05-02T09:08:42Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"170c83726ac08705f5bea821698edaec205370a3f9fc028de2174b11393bc700","abstract_canon_sha256":"3d0d7eb2f9301d59135d93b07d1bc112f16138ad1102c477d2f4cbf820351275"},"schema_version":"1.0"},"canonical_sha256":"a9663e9a034850f1033700d9e6b98272b37adf1dd6ca204f23a01df5642cc057","source":{"kind":"arxiv","id":"1705.00862","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1705.00862","created_at":"2026-05-18T00:25:39Z"},{"alias_kind":"arxiv_version","alias_value":"1705.00862v1","created_at":"2026-05-18T00:25:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.00862","created_at":"2026-05-18T00:25:39Z"},{"alias_kind":"pith_short_12","alias_value":"VFTD5GQDJBIP","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_16","alias_value":"VFTD5GQDJBIPCAZX","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_8","alias_value":"VFTD5GQD","created_at":"2026-05-18T12:31:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:VFTD5GQDJBIPCAZXADM6NOMCOK","target":"record","payload":{"canonical_record":{"source":{"id":"1705.00862","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-05-02T09:08:42Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"170c83726ac08705f5bea821698edaec205370a3f9fc028de2174b11393bc700","abstract_canon_sha256":"3d0d7eb2f9301d59135d93b07d1bc112f16138ad1102c477d2f4cbf820351275"},"schema_version":"1.0"},"canonical_sha256":"a9663e9a034850f1033700d9e6b98272b37adf1dd6ca204f23a01df5642cc057","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:25:39.502601Z","signature_b64":"nJWbCUmm4kd1fZL+jxzQXbQYfGpGjkL7npzocO9m8Wj8i6iBSa15fDAa9VpAbRrEAgEfI/oxnuGIuG51MAwkCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a9663e9a034850f1033700d9e6b98272b37adf1dd6ca204f23a01df5642cc057","last_reissued_at":"2026-05-18T00:25:39.501947Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:25:39.501947Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1705.00862","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":"2026-05-18T00:25:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MepmOwHr/AoQQbgCvg2irrZPD4PKJ1AQDIfGYLY64gmnN+21hDDFGTLSuOY1dEto7f05NT9tOu3iYPR+XvBwCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T20:15:57.522987Z"},"content_sha256":"dfa67aa45f41275ae4c459ea1c6b2e9f38b4ed9d2d8e803c287ea7a3103a4364","schema_version":"1.0","event_id":"sha256:dfa67aa45f41275ae4c459ea1c6b2e9f38b4ed9d2d8e803c287ea7a3103a4364"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:VFTD5GQDJBIPCAZXADM6NOMCOK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Anisotropic Dyonic Black Brane and its Effects on Hydrodynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Bum-Hoon Lee, Chanyong Park, Sunly Khimphun, Yun-Long Zhang","submitted_at":"2017-05-02T09:08:42Z","abstract_excerpt":"We construct $SL(2,R)$ invariant in anisotropic medium, with a dual anisotropic charged black hole geometry in massive gravity. We show how to obtain $SL(2,R)$ elements in terms of new degrees of freedom for Electromagnetic configuration, and construct the general expressions for conductivity with $SL(2,R)$ invariant. The holographic conductivities can be calculated using horizon data in an external magnetic field, and we show the numerical results using the linear response theory."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.00862","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":"2026-05-18T00:25:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RY3L2CuZH6qeSqw+ikc1KRDHpS0lGj6WHHHo0xsRpkmHXq/4QMufQ8rO/tndvRoX/ekgQUxDI9gLi/phalfDAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T20:15:57.523472Z"},"content_sha256":"103d8de63089b4958e1a0f59ff74ef24e17cdd96b101086bdc3defcaf6c37e45","schema_version":"1.0","event_id":"sha256:103d8de63089b4958e1a0f59ff74ef24e17cdd96b101086bdc3defcaf6c37e45"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VFTD5GQDJBIPCAZXADM6NOMCOK/bundle.json","state_url":"https://pith.science/pith/VFTD5GQDJBIPCAZXADM6NOMCOK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VFTD5GQDJBIPCAZXADM6NOMCOK/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":"2026-05-28T20:15:57Z","links":{"resolver":"https://pith.science/pith/VFTD5GQDJBIPCAZXADM6NOMCOK","bundle":"https://pith.science/pith/VFTD5GQDJBIPCAZXADM6NOMCOK/bundle.json","state":"https://pith.science/pith/VFTD5GQDJBIPCAZXADM6NOMCOK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VFTD5GQDJBIPCAZXADM6NOMCOK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:VFTD5GQDJBIPCAZXADM6NOMCOK","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":"3d0d7eb2f9301d59135d93b07d1bc112f16138ad1102c477d2f4cbf820351275","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-05-02T09:08:42Z","title_canon_sha256":"170c83726ac08705f5bea821698edaec205370a3f9fc028de2174b11393bc700"},"schema_version":"1.0","source":{"id":"1705.00862","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1705.00862","created_at":"2026-05-18T00:25:39Z"},{"alias_kind":"arxiv_version","alias_value":"1705.00862v1","created_at":"2026-05-18T00:25:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.00862","created_at":"2026-05-18T00:25:39Z"},{"alias_kind":"pith_short_12","alias_value":"VFTD5GQDJBIP","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_16","alias_value":"VFTD5GQDJBIPCAZX","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_8","alias_value":"VFTD5GQD","created_at":"2026-05-18T12:31:49Z"}],"graph_snapshots":[{"event_id":"sha256:103d8de63089b4958e1a0f59ff74ef24e17cdd96b101086bdc3defcaf6c37e45","target":"graph","created_at":"2026-05-18T00:25:39Z","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 $SL(2,R)$ invariant in anisotropic medium, with a dual anisotropic charged black hole geometry in massive gravity. We show how to obtain $SL(2,R)$ elements in terms of new degrees of freedom for Electromagnetic configuration, and construct the general expressions for conductivity with $SL(2,R)$ invariant. The holographic conductivities can be calculated using horizon data in an external magnetic field, and we show the numerical results using the linear response theory.","authors_text":"Bum-Hoon Lee, Chanyong Park, Sunly Khimphun, Yun-Long Zhang","cross_cats":["gr-qc"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-05-02T09:08:42Z","title":"Anisotropic Dyonic Black Brane and its Effects on Hydrodynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.00862","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:dfa67aa45f41275ae4c459ea1c6b2e9f38b4ed9d2d8e803c287ea7a3103a4364","target":"record","created_at":"2026-05-18T00:25:39Z","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":"3d0d7eb2f9301d59135d93b07d1bc112f16138ad1102c477d2f4cbf820351275","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-05-02T09:08:42Z","title_canon_sha256":"170c83726ac08705f5bea821698edaec205370a3f9fc028de2174b11393bc700"},"schema_version":"1.0","source":{"id":"1705.00862","kind":"arxiv","version":1}},"canonical_sha256":"a9663e9a034850f1033700d9e6b98272b37adf1dd6ca204f23a01df5642cc057","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a9663e9a034850f1033700d9e6b98272b37adf1dd6ca204f23a01df5642cc057","first_computed_at":"2026-05-18T00:25:39.501947Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:25:39.501947Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nJWbCUmm4kd1fZL+jxzQXbQYfGpGjkL7npzocO9m8Wj8i6iBSa15fDAa9VpAbRrEAgEfI/oxnuGIuG51MAwkCg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:25:39.502601Z","signed_message":"canonical_sha256_bytes"},"source_id":"1705.00862","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:dfa67aa45f41275ae4c459ea1c6b2e9f38b4ed9d2d8e803c287ea7a3103a4364","sha256:103d8de63089b4958e1a0f59ff74ef24e17cdd96b101086bdc3defcaf6c37e45"],"state_sha256":"2e42f247e64426e963b56af83b75dda95a2ba3e28128545beaa2cf759c688f1e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zbEUZQJXV9qJj6gJzT1Zo+7qVdiC/bbXFnMA4v9j/65wZ4+UqwK/t0Q64F7t/tQw7T3h7B8ghuYtGcohgbVECg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T20:15:57.527240Z","bundle_sha256":"5a04219514c5a19e66ef8a0a66ba944ad991db259f050efac020f43f3a8bffd4"}}