{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:V6C5NQYKPISFLRHJML2FEFZULZ","short_pith_number":"pith:V6C5NQYK","schema_version":"1.0","canonical_sha256":"af85d6c30a7a2455c4e962f45217345e69b6252a37ba3c80fbe02a050e183627","source":{"kind":"arxiv","id":"1905.03785","version":2},"attestation_state":"computed","paper":{"title":"Misner Gravitational Charges and Variable String Strengths","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Alvaro Ballon Bordo, David Kubiznak, Finnian Gray, Robie A. Hennigar","submitted_at":"2019-05-09T18:00:00Z","abstract_excerpt":"As shown recently (arXiv:1903.08668), consistent thermodynamics of the Lorentzian Taub-NUT solutions with Misner strings present can be formulated provided a new pair of conjugate quantities (related to the NUT parameter) $\\psi-N$ is introduced. In (arXiv:1903.08668) this pair was calculated from the Euclidean action but no geometrical interpretation for the new quantities was provided. In this paper we propose that the potential $\\psi$ should be identified with the surface gravity of the Misner string and the conjugate Misner charge $N$ can be obtained by a Komar-type integration over the tub"},"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":"1905.03785","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-05-09T18:00:00Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"52295efa6acc683bab62bfffad722c33bf8ba2ab27d95654605f38805b25aab3","abstract_canon_sha256":"d107eb0aade878539b62397ee8a4d1e14fcd4d9d1c2ca2bfd00271de71fc5231"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:31:04.068545Z","signature_b64":"dbpLDp02+LOfsp6xq7jxCguJ0M/6EPZYdkfEBU7Sqd18eOSozNXrJMnr2ov4uunvOnw9QqzoIyBAqvUlG+QeDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"af85d6c30a7a2455c4e962f45217345e69b6252a37ba3c80fbe02a050e183627","last_reissued_at":"2026-07-05T00:31:04.068041Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:31:04.068041Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Misner Gravitational Charges and Variable String Strengths","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Alvaro Ballon Bordo, David Kubiznak, Finnian Gray, Robie A. Hennigar","submitted_at":"2019-05-09T18:00:00Z","abstract_excerpt":"As shown recently (arXiv:1903.08668), consistent thermodynamics of the Lorentzian Taub-NUT solutions with Misner strings present can be formulated provided a new pair of conjugate quantities (related to the NUT parameter) $\\psi-N$ is introduced. In (arXiv:1903.08668) this pair was calculated from the Euclidean action but no geometrical interpretation for the new quantities was provided. In this paper we propose that the potential $\\psi$ should be identified with the surface gravity of the Misner string and the conjugate Misner charge $N$ can be obtained by a Komar-type integration over the tub"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1905.03785","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1905.03785/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":"1905.03785","created_at":"2026-07-05T00:31:04.068095+00:00"},{"alias_kind":"arxiv_version","alias_value":"1905.03785v2","created_at":"2026-07-05T00:31:04.068095+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1905.03785","created_at":"2026-07-05T00:31:04.068095+00:00"},{"alias_kind":"pith_short_12","alias_value":"V6C5NQYKPISF","created_at":"2026-07-05T00:31:04.068095+00:00"},{"alias_kind":"pith_short_16","alias_value":"V6C5NQYKPISFLRHJ","created_at":"2026-07-05T00:31:04.068095+00:00"},{"alias_kind":"pith_short_8","alias_value":"V6C5NQYK","created_at":"2026-07-05T00:31:04.068095+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.03958","citing_title":"Multihair thermodynamics of Kerr-Newman-NUT-AdS$_4$ spacetimes","ref_index":20,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/V6C5NQYKPISFLRHJML2FEFZULZ","json":"https://pith.science/pith/V6C5NQYKPISFLRHJML2FEFZULZ.json","graph_json":"https://pith.science/api/pith-number/V6C5NQYKPISFLRHJML2FEFZULZ/graph.json","events_json":"https://pith.science/api/pith-number/V6C5NQYKPISFLRHJML2FEFZULZ/events.json","paper":"https://pith.science/paper/V6C5NQYK"},"agent_actions":{"view_html":"https://pith.science/pith/V6C5NQYKPISFLRHJML2FEFZULZ","download_json":"https://pith.science/pith/V6C5NQYKPISFLRHJML2FEFZULZ.json","view_paper":"https://pith.science/paper/V6C5NQYK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1905.03785&json=true","fetch_graph":"https://pith.science/api/pith-number/V6C5NQYKPISFLRHJML2FEFZULZ/graph.json","fetch_events":"https://pith.science/api/pith-number/V6C5NQYKPISFLRHJML2FEFZULZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/V6C5NQYKPISFLRHJML2FEFZULZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/V6C5NQYKPISFLRHJML2FEFZULZ/action/storage_attestation","attest_author":"https://pith.science/pith/V6C5NQYKPISFLRHJML2FEFZULZ/action/author_attestation","sign_citation":"https://pith.science/pith/V6C5NQYKPISFLRHJML2FEFZULZ/action/citation_signature","submit_replication":"https://pith.science/pith/V6C5NQYKPISFLRHJML2FEFZULZ/action/replication_record"}},"created_at":"2026-07-05T00:31:04.068095+00:00","updated_at":"2026-07-05T00:31:04.068095+00:00"}