{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:FFGKREY2JFHQ5QKYMVSCF6C4RK","short_pith_number":"pith:FFGKREY2","schema_version":"1.0","canonical_sha256":"294ca8931a494f0ec158656422f85c8aa2ad0853b1cab3536941e2f8fa385544","source":{"kind":"arxiv","id":"2608.02196","version":1},"attestation_state":"computed","paper":{"title":"Charged Black Holes with a Lorentz--Violating Kalb--Ramond Background","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Jia-Hui Yang, Jia-Zhou Liu, Xin-Yu Guo, Yu-Xiao Liu","submitted_at":"2026-08-03T13:18:06Z","abstract_excerpt":"We investigate exact static, spherically symmetric electrically charged black hole solutions in a gravitational theory with spontaneous Lorentz-symmetry breaking induced by a background Kalb--Ramond field. In contrast to previous analyses that retained only one nonminimal curvature coupling, we include the combined effects of the two independent nonminimal curvature couplings and obtain charged black hole solutions both with and without a cosmological constant. Using the Iyer--Wald covariant phase-space formalism, we derive the corrected thermodynamic quantities and analyze the Joule--Thomson "},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2608.02196","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2026-08-03T13:18:06Z","cross_cats_sorted":[],"title_canon_sha256":"826e5982b988e54a6932b6cb0fa501e5f81e2f75642246dbca34f0c370fb8706","abstract_canon_sha256":"986f8882311be85b56e87859e37226779a89d16c450acf4c13d6b74f644479f2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-08-04T02:11:23.022914Z","signature_b64":"qRFFyzd9lxTE7fV0VnvsrNngO4Es90Ve8M/ojFP25cnUCip8i34F8iZ7dmuDrYmtKL+m1h1lVuFkcetd2kp6Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"294ca8931a494f0ec158656422f85c8aa2ad0853b1cab3536941e2f8fa385544","last_reissued_at":"2026-08-04T02:11:23.021099Z","signature_status":"signed_v1","first_computed_at":"2026-08-04T02:11:23.021099Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Charged Black Holes with a Lorentz--Violating Kalb--Ramond Background","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Jia-Hui Yang, Jia-Zhou Liu, Xin-Yu Guo, Yu-Xiao Liu","submitted_at":"2026-08-03T13:18:06Z","abstract_excerpt":"We investigate exact static, spherically symmetric electrically charged black hole solutions in a gravitational theory with spontaneous Lorentz-symmetry breaking induced by a background Kalb--Ramond field. In contrast to previous analyses that retained only one nonminimal curvature coupling, we include the combined effects of the two independent nonminimal curvature couplings and obtain charged black hole solutions both with and without a cosmological constant. Using the Iyer--Wald covariant phase-space formalism, we derive the corrected thermodynamic quantities and analyze the Joule--Thomson "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2608.02196","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2608.02196/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2608.02196","created_at":"2026-08-04T02:11:23.022843+00:00"},{"alias_kind":"arxiv_version","alias_value":"2608.02196v1","created_at":"2026-08-04T02:11:23.022843+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2608.02196","created_at":"2026-08-04T02:11:23.022843+00:00"},{"alias_kind":"pith_short_12","alias_value":"FFGKREY2JFHQ","created_at":"2026-08-04T02:11:23.022843+00:00"},{"alias_kind":"pith_short_16","alias_value":"FFGKREY2JFHQ5QKY","created_at":"2026-08-04T02:11:23.022843+00:00"},{"alias_kind":"pith_short_8","alias_value":"FFGKREY2","created_at":"2026-08-04T02:11:23.022843+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FFGKREY2JFHQ5QKYMVSCF6C4RK","json":"https://pith.science/pith/FFGKREY2JFHQ5QKYMVSCF6C4RK.json","graph_json":"https://pith.science/api/pith-number/FFGKREY2JFHQ5QKYMVSCF6C4RK/graph.json","events_json":"https://pith.science/api/pith-number/FFGKREY2JFHQ5QKYMVSCF6C4RK/events.json","paper":"https://pith.science/paper/FFGKREY2"},"agent_actions":{"view_html":"https://pith.science/pith/FFGKREY2JFHQ5QKYMVSCF6C4RK","download_json":"https://pith.science/pith/FFGKREY2JFHQ5QKYMVSCF6C4RK.json","view_paper":"https://pith.science/paper/FFGKREY2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2608.02196&json=true","fetch_graph":"https://pith.science/api/pith-number/FFGKREY2JFHQ5QKYMVSCF6C4RK/graph.json","fetch_events":"https://pith.science/api/pith-number/FFGKREY2JFHQ5QKYMVSCF6C4RK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FFGKREY2JFHQ5QKYMVSCF6C4RK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FFGKREY2JFHQ5QKYMVSCF6C4RK/action/storage_attestation","attest_author":"https://pith.science/pith/FFGKREY2JFHQ5QKYMVSCF6C4RK/action/author_attestation","sign_citation":"https://pith.science/pith/FFGKREY2JFHQ5QKYMVSCF6C4RK/action/citation_signature","submit_replication":"https://pith.science/pith/FFGKREY2JFHQ5QKYMVSCF6C4RK/action/replication_record"}},"created_at":"2026-08-04T02:11:23.022843+00:00","updated_at":"2026-08-04T02:11:23.022843+00:00"}