{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:LSOFHJOJRZK7UMRUR4LNRP4NTN","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":"c82aa18b7ef782bcc47fad7ae008997ee819182c76167bbac30343abf9751373","cross_cats_sorted":["astro-ph.HE","hep-th","math-ph","math.MP"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2025-01-17T01:05:58Z","title_canon_sha256":"87c786a83b8a21b20d9088a089d8638d2f4d7c962c878194dea58803586755f7"},"schema_version":"1.0","source":{"id":"2501.09899","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2501.09899","created_at":"2026-07-05T10:46:22Z"},{"alias_kind":"arxiv_version","alias_value":"2501.09899v2","created_at":"2026-07-05T10:46:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.09899","created_at":"2026-07-05T10:46:22Z"},{"alias_kind":"pith_short_12","alias_value":"LSOFHJOJRZK7","created_at":"2026-07-05T10:46:22Z"},{"alias_kind":"pith_short_16","alias_value":"LSOFHJOJRZK7UMRU","created_at":"2026-07-05T10:46:22Z"},{"alias_kind":"pith_short_8","alias_value":"LSOFHJOJ","created_at":"2026-07-05T10:46:22Z"}],"graph_snapshots":[{"event_id":"sha256:c33f628273f61cf1d82a296d721249d292ef0fbe12057334deda8bec6ed597f0","target":"graph","created_at":"2026-07-05T10:46:22Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2501.09899/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In this study, we explore a static, spherically symmetric black hole solution in the context of a self-interacting Kalb-Ramond field coupled with a global monopole. By incorporating the effects of Lorentz-violating term $\\ell$ and the monopole charge $\\eta$ in the KR field, we derive the modified gravitational field equations and analyze the resulting black hole spacetime. The obtained solution exhibits deviations from the Schwarzschild metric with topological defect, as it is influenced by the monopole charge and self-interaction potential. We investigate the thermodynamic properties of the b","authors_text":"Ali \\\"Ovg\\\"un, Mohsen Fathi","cross_cats":["astro-ph.HE","hep-th","math-ph","math.MP"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2025-01-17T01:05:58Z","title":"Black hole with global monopole charge in self-interacting Kalb-Ramond field"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2501.09899","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":"sha256:2140b5fcf9119efdb2246a3fca4ca278320e76866e919dc957d29b4f54ad3862","target":"record","created_at":"2026-07-05T10:46:22Z","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":"c82aa18b7ef782bcc47fad7ae008997ee819182c76167bbac30343abf9751373","cross_cats_sorted":["astro-ph.HE","hep-th","math-ph","math.MP"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2025-01-17T01:05:58Z","title_canon_sha256":"87c786a83b8a21b20d9088a089d8638d2f4d7c962c878194dea58803586755f7"},"schema_version":"1.0","source":{"id":"2501.09899","kind":"arxiv","version":2}},"canonical_sha256":"5c9c53a5c98e55fa32348f16d8bf8d9b4bcc350cec61b5763e87cf61436a2d8a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5c9c53a5c98e55fa32348f16d8bf8d9b4bcc350cec61b5763e87cf61436a2d8a","first_computed_at":"2026-07-05T10:46:22.437679Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:46:22.437679Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"v8tQQMdeGXr41qIlqqpqs4bVT7xjZfiP2ZbjveqzeWLac1CB4KoqlNJAvJms79A+9nVOQSeg3O9s4vrctC3rAA==","signature_status":"signed_v1","signed_at":"2026-07-05T10:46:22.438177Z","signed_message":"canonical_sha256_bytes"},"source_id":"2501.09899","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2140b5fcf9119efdb2246a3fca4ca278320e76866e919dc957d29b4f54ad3862","sha256:c33f628273f61cf1d82a296d721249d292ef0fbe12057334deda8bec6ed597f0"],"state_sha256":"147706981d2d3b9072fcd8fa856a57e0515d559ba65e88a0fc5215e7cf577d0e"}