{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:JPUO6HE6F7CYTKGL2SQPPUCVVM","short_pith_number":"pith:JPUO6HE6","schema_version":"1.0","canonical_sha256":"4be8ef1c9e2fc589a8cbd4a0f7d055ab22854b4dc19647444a432bfd9aa8a6e1","source":{"kind":"arxiv","id":"hep-th/9612015","version":1},"attestation_state":"computed","paper":{"title":"Dipole Moments of Black Holes and String States","license":"","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"J. Rahmfeld, J.T. Liu, M.J. Duff","submitted_at":"1996-12-02T20:09:27Z","abstract_excerpt":"As a further test of the conjectured equivalence of string states and extremal black holes, we compute the dipole moments of black holes with arbitrary spin and superspin in D=4,N=4 supergravity coupled to 22 vector multiplets and compare them with the dipole moments of states in the heterotic string on $T^6$ or the Type IIA string on $K3 \\times T^2$. Starting from a purely bosonic black hole with Kerr angular momentum L, the superpartners are generated by acting with fermion zero modes, thus filling out the complete supermultiplet. $L$ is then identified with the superspin. On the heterotic s"},"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":"hep-th/9612015","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1996-12-02T20:09:27Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"05d43d47560f2840b5639d37e2b2e058011ec609a639f1412f5f352bf0e21338","abstract_canon_sha256":"42da4ea9685a67d3e26f04917a78182a1242197085bcb35c3befe56b46c59542"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:02:26.537740Z","signature_b64":"w2KaDx0aJNDzdTo+PVpxXrBJHaJxMnJS4BKVXR2hswzRr79vT9RI0Er0ihTHPeVceCD7KMU4kdXvR5Pk5tzZDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4be8ef1c9e2fc589a8cbd4a0f7d055ab22854b4dc19647444a432bfd9aa8a6e1","last_reissued_at":"2026-07-04T16:02:26.537386Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:02:26.537386Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dipole Moments of Black Holes and String States","license":"","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"J. Rahmfeld, J.T. Liu, M.J. Duff","submitted_at":"1996-12-02T20:09:27Z","abstract_excerpt":"As a further test of the conjectured equivalence of string states and extremal black holes, we compute the dipole moments of black holes with arbitrary spin and superspin in D=4,N=4 supergravity coupled to 22 vector multiplets and compare them with the dipole moments of states in the heterotic string on $T^6$ or the Type IIA string on $K3 \\times T^2$. Starting from a purely bosonic black hole with Kerr angular momentum L, the superpartners are generated by acting with fermion zero modes, thus filling out the complete supermultiplet. $L$ is then identified with the superspin. On the heterotic s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9612015","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/hep-th/9612015/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":"hep-th/9612015","created_at":"2026-07-04T16:02:26.537442+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9612015v1","created_at":"2026-07-04T16:02:26.537442+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9612015","created_at":"2026-07-04T16:02:26.537442+00:00"},{"alias_kind":"pith_short_12","alias_value":"JPUO6HE6F7CY","created_at":"2026-07-04T16:02:26.537442+00:00"},{"alias_kind":"pith_short_16","alias_value":"JPUO6HE6F7CYTKGL","created_at":"2026-07-04T16:02:26.537442+00:00"},{"alias_kind":"pith_short_8","alias_value":"JPUO6HE6","created_at":"2026-07-04T16:02:26.537442+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/JPUO6HE6F7CYTKGL2SQPPUCVVM","json":"https://pith.science/pith/JPUO6HE6F7CYTKGL2SQPPUCVVM.json","graph_json":"https://pith.science/api/pith-number/JPUO6HE6F7CYTKGL2SQPPUCVVM/graph.json","events_json":"https://pith.science/api/pith-number/JPUO6HE6F7CYTKGL2SQPPUCVVM/events.json","paper":"https://pith.science/paper/JPUO6HE6"},"agent_actions":{"view_html":"https://pith.science/pith/JPUO6HE6F7CYTKGL2SQPPUCVVM","download_json":"https://pith.science/pith/JPUO6HE6F7CYTKGL2SQPPUCVVM.json","view_paper":"https://pith.science/paper/JPUO6HE6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9612015&json=true","fetch_graph":"https://pith.science/api/pith-number/JPUO6HE6F7CYTKGL2SQPPUCVVM/graph.json","fetch_events":"https://pith.science/api/pith-number/JPUO6HE6F7CYTKGL2SQPPUCVVM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JPUO6HE6F7CYTKGL2SQPPUCVVM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JPUO6HE6F7CYTKGL2SQPPUCVVM/action/storage_attestation","attest_author":"https://pith.science/pith/JPUO6HE6F7CYTKGL2SQPPUCVVM/action/author_attestation","sign_citation":"https://pith.science/pith/JPUO6HE6F7CYTKGL2SQPPUCVVM/action/citation_signature","submit_replication":"https://pith.science/pith/JPUO6HE6F7CYTKGL2SQPPUCVVM/action/replication_record"}},"created_at":"2026-07-04T16:02:26.537442+00:00","updated_at":"2026-07-04T16:02:26.537442+00:00"}