{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:P5TTDI75J3C7CLCNYH3HNQ6SAJ","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":"849fd10b63bda2f864daa4ddcf4e4a140152f7b9a3c1f17ccb8fcddbac26d3fd","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-04-09T16:38:57Z","title_canon_sha256":"cc064ccfb7ee8d442de301317d6c208dae33d003e6e7654c5e23b0a3d8c8b867"},"schema_version":"1.0","source":{"id":"2604.08441","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2604.08441","created_at":"2026-06-02T03:04:41Z"},{"alias_kind":"arxiv_version","alias_value":"2604.08441v2","created_at":"2026-06-02T03:04:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2604.08441","created_at":"2026-06-02T03:04:41Z"},{"alias_kind":"pith_short_12","alias_value":"P5TTDI75J3C7","created_at":"2026-06-02T03:04:41Z"},{"alias_kind":"pith_short_16","alias_value":"P5TTDI75J3C7CLCN","created_at":"2026-06-02T03:04:41Z"},{"alias_kind":"pith_short_8","alias_value":"P5TTDI75","created_at":"2026-06-02T03:04:41Z"}],"graph_snapshots":[{"event_id":"sha256:2638ef6f38b0af29293527afea2a6a573c0827247983d74c5952eebf28e51d19","target":"graph","created_at":"2026-06-02T03:04:41Z","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":4,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","text":"For each model, exact solutions for the metric, scalar field, gauge fields, and coupling functions are derived, incorporating anisotropic scaling exponents and general warp factors, including Gaussian forms. ... We show that the third law of thermodynamics, which requires entropy to vanish as temperature approaches zero, is satisfied for a certain range of parameters in both models. However, for specific warp factors or coupling constants, the entropy-temperature relation exhibits non-monotonic or multi-valued behavior, suggesting the possibility of phase transitions and a violation of the third law."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"That specific scalar potentials and field coupling functions can be chosen to admit exact solutions with the desired Lifshitz asymptotics and general warp factors in arbitrary dimensions, while correctly yielding the thermodynamic quantities used to test the third law."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"Exact black brane solutions with Lifshitz asymptotics are derived in arbitrary dimensions for two models, satisfying the third law for some parameters but exhibiting non-monotonic entropy-temperature relations for others."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"Exact Lifshitz-like black brane solutions in arbitrary dimensions satisfy the third law of thermodynamics only for certain choices of warp factors and couplings."}],"snapshot_sha256":"672783e0bce6645759bfcf5f1a1f2660d7737b90e30d90a4de9cfbf3c8334b98"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2604.08441/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In this paper we present a systematic construction of an(isotropic) black brane solutions in arbitrary spacetime dimensions $D$ in particular, with Lifshitz-like asymptotics. Two distinct holographic models are considered. The first model involves a scalar field with a potential coupled to two Maxwell fields, allowing for both electric and magnetic charges. The second model includes a scalar field, a Maxwell field, and a three-form field strength of a Kalb-Ramond field. For each model, exact solutions for the metric, scalar field, gauge fields, and coupling functions are derived, incorporating","authors_text":"Anastasia A. Golubtsova, Irina Ya. Aref'eva, Valeriya D. Nerovnova","cross_cats":["gr-qc"],"headline":"Exact Lifshitz-like black brane solutions in arbitrary dimensions satisfy the third law of thermodynamics only for certain choices of warp factors and couplings.","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-04-09T16:38:57Z","title":"Lifshitz-like black branes in arbitrary dimensions and the third law of thermodynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2604.08441","kind":"arxiv","version":2},"verdict":{"created_at":"2026-05-10T17:36:22.589829Z","id":"110b4bae-3881-4144-90fb-594631f4c6dc","model_set":{"reader":"grok-4.3"},"one_line_summary":"Exact black brane solutions with Lifshitz asymptotics are derived in arbitrary dimensions for two models, satisfying the third law for some parameters but exhibiting non-monotonic entropy-temperature relations for others.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"Exact Lifshitz-like black brane solutions in arbitrary dimensions satisfy the third law of thermodynamics only for certain choices of warp factors and couplings.","strongest_claim":"For each model, exact solutions for the metric, scalar field, gauge fields, and coupling functions are derived, incorporating anisotropic scaling exponents and general warp factors, including Gaussian forms. ... We show that the third law of thermodynamics, which requires entropy to vanish as temperature approaches zero, is satisfied for a certain range of parameters in both models. However, for specific warp factors or coupling constants, the entropy-temperature relation exhibits non-monotonic or multi-valued behavior, suggesting the possibility of phase transitions and a violation of the third law.","weakest_assumption":"That specific scalar potentials and field coupling functions can be chosen to admit exact solutions with the desired Lifshitz asymptotics and general warp factors in arbitrary dimensions, while correctly yielding the thermodynamic quantities used to test the third law."}},"verdict_id":"110b4bae-3881-4144-90fb-594631f4c6dc"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:0dfb049f31ef9e3714c70fef96b81e5dc3c8c1b263079681889e20681e064635","target":"record","created_at":"2026-06-02T03:04:41Z","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":"849fd10b63bda2f864daa4ddcf4e4a140152f7b9a3c1f17ccb8fcddbac26d3fd","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-04-09T16:38:57Z","title_canon_sha256":"cc064ccfb7ee8d442de301317d6c208dae33d003e6e7654c5e23b0a3d8c8b867"},"schema_version":"1.0","source":{"id":"2604.08441","kind":"arxiv","version":2}},"canonical_sha256":"7f6731a3fd4ec5f12c4dc1f676c3d202641d8ab8c4f403c830944d1915bd97a7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7f6731a3fd4ec5f12c4dc1f676c3d202641d8ab8c4f403c830944d1915bd97a7","first_computed_at":"2026-06-02T03:04:41.000990Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-02T03:04:41.000990Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nvOc8feKdBpUwS8s4bSK7q2iBGL3SrKuz3gZF1+80fc3kQ0JIXt9Lb5jQ/iKOGkZToj48qEqLm6l+/RWcxWGCA==","signature_status":"signed_v1","signed_at":"2026-06-02T03:04:41.001469Z","signed_message":"canonical_sha256_bytes"},"source_id":"2604.08441","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0dfb049f31ef9e3714c70fef96b81e5dc3c8c1b263079681889e20681e064635","sha256:2638ef6f38b0af29293527afea2a6a573c0827247983d74c5952eebf28e51d19"],"state_sha256":"13eba1c83611ae803bd95f6f03699f683b800960357d89eabb4607b5774ef011"}