{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:ABF7W6NHQVCDI26U6XGKPYIVBF","short_pith_number":"pith:ABF7W6NH","canonical_record":{"source":{"id":"1106.1637","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-06-08T19:53:42Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"e1396d12e2e11d0e5bb6c10f107829ec8b150cd45415a909f15581d90f02e6eb","abstract_canon_sha256":"835f78fcdf4a9d0bb72d87e85aa1a21e98d0823783b702275272ae02b68f192f"},"schema_version":"1.0"},"canonical_sha256":"004bfb79a78544346bd4f5cca7e1150978f69c2fca60636523473c8f926284fb","source":{"kind":"arxiv","id":"1106.1637","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1106.1637","created_at":"2026-05-18T04:08:45Z"},{"alias_kind":"arxiv_version","alias_value":"1106.1637v2","created_at":"2026-05-18T04:08:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.1637","created_at":"2026-05-18T04:08:45Z"},{"alias_kind":"pith_short_12","alias_value":"ABF7W6NHQVCD","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_16","alias_value":"ABF7W6NHQVCDI26U","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_8","alias_value":"ABF7W6NH","created_at":"2026-05-18T12:26:24Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:ABF7W6NHQVCDI26U6XGKPYIVBF","target":"record","payload":{"canonical_record":{"source":{"id":"1106.1637","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-06-08T19:53:42Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"e1396d12e2e11d0e5bb6c10f107829ec8b150cd45415a909f15581d90f02e6eb","abstract_canon_sha256":"835f78fcdf4a9d0bb72d87e85aa1a21e98d0823783b702275272ae02b68f192f"},"schema_version":"1.0"},"canonical_sha256":"004bfb79a78544346bd4f5cca7e1150978f69c2fca60636523473c8f926284fb","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:08:45.124574Z","signature_b64":"v48llvR5m19VJDfhvLimV2/5eegrndo0zBnfBOpTjxxg4MIq7tAQ1h48h3WXx9xPfJ4ENmRBVhKnUjwCLA3nDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"004bfb79a78544346bd4f5cca7e1150978f69c2fca60636523473c8f926284fb","last_reissued_at":"2026-05-18T04:08:45.124000Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:08:45.124000Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1106.1637","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":"2026-05-18T04:08:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QcW8IXOzzrxNJUwkvu3xZwLR0VbrzxafTqL4CQHcAS7zxwySEPGjCy9V/h1xgDJWOzgo1+yymto4e22MDlCzBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T21:38:41.317422Z"},"content_sha256":"0a90bb7a32ce0bd5e334203d4592dc48a084fb303adfbb1f932d9e768b045615","schema_version":"1.0","event_id":"sha256:0a90bb7a32ce0bd5e334203d4592dc48a084fb303adfbb1f932d9e768b045615"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:ABF7W6NHQVCDI26U6XGKPYIVBF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Thermodynamics and Instabilities of a Strongly Coupled Anisotropic Plasma","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-th","authors_text":"David Mateos, Diego Trancanelli","submitted_at":"2011-06-08T19:53:42Z","abstract_excerpt":"We extend our analysis of a IIB supergravity solution dual to a spatially anisotropic finite-temperature N=4 super Yang-Mills plasma. The solution is static, possesses an anisotropic horizon, and is completely regular. The full geometry can be viewed as a renormalization group flow from an AdS geometry in the ultraviolet to a Lifshitz-like geometry in the infrared. The anisotropy can be equivalently understood as resulting from a position-dependent theta-term or from a non-zero number density of dissolved D7-branes. The holographic stress tensor is conserved and anisotropic. The presence of a "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.1637","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":"2026-05-18T04:08:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1Wwp/P0oB9MPpFcsrTqX3CEFMWEbPDSXIauX0gxXBRvaOGookp5x4soqDMepVFtoLNCxIj1YaURl8kwCjYXODw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T21:38:41.317763Z"},"content_sha256":"8379c4f6b8d5604a77b141060171151c0a46346c35542ed934c373bd9f2c26b6","schema_version":"1.0","event_id":"sha256:8379c4f6b8d5604a77b141060171151c0a46346c35542ed934c373bd9f2c26b6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ABF7W6NHQVCDI26U6XGKPYIVBF/bundle.json","state_url":"https://pith.science/pith/ABF7W6NHQVCDI26U6XGKPYIVBF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ABF7W6NHQVCDI26U6XGKPYIVBF/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":"2026-05-20T21:38:41Z","links":{"resolver":"https://pith.science/pith/ABF7W6NHQVCDI26U6XGKPYIVBF","bundle":"https://pith.science/pith/ABF7W6NHQVCDI26U6XGKPYIVBF/bundle.json","state":"https://pith.science/pith/ABF7W6NHQVCDI26U6XGKPYIVBF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ABF7W6NHQVCDI26U6XGKPYIVBF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:ABF7W6NHQVCDI26U6XGKPYIVBF","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":"835f78fcdf4a9d0bb72d87e85aa1a21e98d0823783b702275272ae02b68f192f","cross_cats_sorted":["hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-06-08T19:53:42Z","title_canon_sha256":"e1396d12e2e11d0e5bb6c10f107829ec8b150cd45415a909f15581d90f02e6eb"},"schema_version":"1.0","source":{"id":"1106.1637","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1106.1637","created_at":"2026-05-18T04:08:45Z"},{"alias_kind":"arxiv_version","alias_value":"1106.1637v2","created_at":"2026-05-18T04:08:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.1637","created_at":"2026-05-18T04:08:45Z"},{"alias_kind":"pith_short_12","alias_value":"ABF7W6NHQVCD","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_16","alias_value":"ABF7W6NHQVCDI26U","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_8","alias_value":"ABF7W6NH","created_at":"2026-05-18T12:26:24Z"}],"graph_snapshots":[{"event_id":"sha256:8379c4f6b8d5604a77b141060171151c0a46346c35542ed934c373bd9f2c26b6","target":"graph","created_at":"2026-05-18T04:08:45Z","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 extend our analysis of a IIB supergravity solution dual to a spatially anisotropic finite-temperature N=4 super Yang-Mills plasma. The solution is static, possesses an anisotropic horizon, and is completely regular. The full geometry can be viewed as a renormalization group flow from an AdS geometry in the ultraviolet to a Lifshitz-like geometry in the infrared. The anisotropy can be equivalently understood as resulting from a position-dependent theta-term or from a non-zero number density of dissolved D7-branes. The holographic stress tensor is conserved and anisotropic. The presence of a ","authors_text":"David Mateos, Diego Trancanelli","cross_cats":["hep-ph","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-06-08T19:53:42Z","title":"Thermodynamics and Instabilities of a Strongly Coupled Anisotropic Plasma"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.1637","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":"sha256:0a90bb7a32ce0bd5e334203d4592dc48a084fb303adfbb1f932d9e768b045615","target":"record","created_at":"2026-05-18T04:08:45Z","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":"835f78fcdf4a9d0bb72d87e85aa1a21e98d0823783b702275272ae02b68f192f","cross_cats_sorted":["hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-06-08T19:53:42Z","title_canon_sha256":"e1396d12e2e11d0e5bb6c10f107829ec8b150cd45415a909f15581d90f02e6eb"},"schema_version":"1.0","source":{"id":"1106.1637","kind":"arxiv","version":2}},"canonical_sha256":"004bfb79a78544346bd4f5cca7e1150978f69c2fca60636523473c8f926284fb","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"004bfb79a78544346bd4f5cca7e1150978f69c2fca60636523473c8f926284fb","first_computed_at":"2026-05-18T04:08:45.124000Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:08:45.124000Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"v48llvR5m19VJDfhvLimV2/5eegrndo0zBnfBOpTjxxg4MIq7tAQ1h48h3WXx9xPfJ4ENmRBVhKnUjwCLA3nDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T04:08:45.124574Z","signed_message":"canonical_sha256_bytes"},"source_id":"1106.1637","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0a90bb7a32ce0bd5e334203d4592dc48a084fb303adfbb1f932d9e768b045615","sha256:8379c4f6b8d5604a77b141060171151c0a46346c35542ed934c373bd9f2c26b6"],"state_sha256":"205f7409101189fa7a68e25f90cf7f85a43fcaa6a76be46059185a855e48f22c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Wc6mlmJ/u/3bkb8Xycux6ExvK9FLL+XRIdw0fEZ4ghsbVHkIIkIhvOnav0gkJlsoWwChKlTuvEShDbHmy6uNBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-20T21:38:41.319832Z","bundle_sha256":"13108becb558dfaffa488e4eb7053b0b2b10afa13be155e5779b5bf267fca781"}}