{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:PXFMABLMDI7S2XFUVIYZWGVDJK","short_pith_number":"pith:PXFMABLM","schema_version":"1.0","canonical_sha256":"7dcac0056c1a3f2d5cb4aa319b1aa34a8989bd34afd0d8a13385e5f998b2b8a7","source":{"kind":"arxiv","id":"1905.06350","version":2},"attestation_state":"computed","paper":{"title":"The First Law for Rotating NUTs","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":"2019-05-15T18:00:11Z","abstract_excerpt":"We address a long-standing problem of describing the thermodynamics of rotating Taub--NUT solutions. The obtained first law is of full cohomogeneity and allows for asymmetric distributions of Misner strings as well as their potential variable strengths---encoded in the gravitational Misner charges. Notably, the angular momentum is no longer given by the Noether charge over the sphere at infinity and picks up non-trivial contributions from Misner strings."},"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":"1905.06350","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-05-15T18:00:11Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"a6a76f30a7e255941e3d23de12714a8a9f75845ffc233963085450ff23ef2265","abstract_canon_sha256":"4a337ad9ceb4748aca82a5eb8cd345dfd5997cea0c4dccc7915f100272340332"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:06:43.704885Z","signature_b64":"dUl6F+6mnn3aqKpfmOIF4zeIVv4dH8motiMi7tG4Sjf86rA9CaA0t18MbmtRqpvafkTTuYA8540fjwQMOHxhAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7dcac0056c1a3f2d5cb4aa319b1aa34a8989bd34afd0d8a13385e5f998b2b8a7","last_reissued_at":"2026-07-05T00:06:43.704448Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:06:43.704448Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The First Law for Rotating NUTs","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":"2019-05-15T18:00:11Z","abstract_excerpt":"We address a long-standing problem of describing the thermodynamics of rotating Taub--NUT solutions. The obtained first law is of full cohomogeneity and allows for asymmetric distributions of Misner strings as well as their potential variable strengths---encoded in the gravitational Misner charges. Notably, the angular momentum is no longer given by the Noether charge over the sphere at infinity and picks up non-trivial contributions from Misner strings."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1905.06350","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/1905.06350/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":"1905.06350","created_at":"2026-07-05T00:06:43.704504+00:00"},{"alias_kind":"arxiv_version","alias_value":"1905.06350v2","created_at":"2026-07-05T00:06:43.704504+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1905.06350","created_at":"2026-07-05T00:06:43.704504+00:00"},{"alias_kind":"pith_short_12","alias_value":"PXFMABLMDI7S","created_at":"2026-07-05T00:06:43.704504+00:00"},{"alias_kind":"pith_short_16","alias_value":"PXFMABLMDI7S2XFU","created_at":"2026-07-05T00:06:43.704504+00:00"},{"alias_kind":"pith_short_8","alias_value":"PXFMABLM","created_at":"2026-07-05T00:06:43.704504+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.03958","citing_title":"Multihair thermodynamics of Kerr-Newman-NUT-AdS$_4$ spacetimes","ref_index":21,"is_internal_anchor":false},{"citing_arxiv_id":"2606.30507","citing_title":"The Role of the Volume in Black Hole Thermodynamics","ref_index":16,"is_internal_anchor":false},{"citing_arxiv_id":"2602.01111","citing_title":"Charged nutty black holes are hairy","ref_index":11,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PXFMABLMDI7S2XFUVIYZWGVDJK","json":"https://pith.science/pith/PXFMABLMDI7S2XFUVIYZWGVDJK.json","graph_json":"https://pith.science/api/pith-number/PXFMABLMDI7S2XFUVIYZWGVDJK/graph.json","events_json":"https://pith.science/api/pith-number/PXFMABLMDI7S2XFUVIYZWGVDJK/events.json","paper":"https://pith.science/paper/PXFMABLM"},"agent_actions":{"view_html":"https://pith.science/pith/PXFMABLMDI7S2XFUVIYZWGVDJK","download_json":"https://pith.science/pith/PXFMABLMDI7S2XFUVIYZWGVDJK.json","view_paper":"https://pith.science/paper/PXFMABLM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1905.06350&json=true","fetch_graph":"https://pith.science/api/pith-number/PXFMABLMDI7S2XFUVIYZWGVDJK/graph.json","fetch_events":"https://pith.science/api/pith-number/PXFMABLMDI7S2XFUVIYZWGVDJK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PXFMABLMDI7S2XFUVIYZWGVDJK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PXFMABLMDI7S2XFUVIYZWGVDJK/action/storage_attestation","attest_author":"https://pith.science/pith/PXFMABLMDI7S2XFUVIYZWGVDJK/action/author_attestation","sign_citation":"https://pith.science/pith/PXFMABLMDI7S2XFUVIYZWGVDJK/action/citation_signature","submit_replication":"https://pith.science/pith/PXFMABLMDI7S2XFUVIYZWGVDJK/action/replication_record"}},"created_at":"2026-07-05T00:06:43.704504+00:00","updated_at":"2026-07-05T00:06:43.704504+00:00"}