{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:RCAFCDRGCHC25M4HUEH7MD3FT5","short_pith_number":"pith:RCAFCDRG","schema_version":"1.0","canonical_sha256":"8880510e2611c5aeb387a10ff60f659f425902b47846b33fa650420701cfe1b8","source":{"kind":"arxiv","id":"2412.14822","version":2},"attestation_state":"computed","paper":{"title":"$\\mathcal{N}=2$ superconformal gravitino in harmonic superspace","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Evgeny Ivanov, Nikita Zaigraev","submitted_at":"2024-12-19T13:13:17Z","abstract_excerpt":"We present the harmonic superspace formulation of $\\mathcal{N}=2$ gravitino multiplet, the simplest $\\mathcal{N}=2$ half-integer spin gauge supermultiplet. It is shown that, quite similar to other $\\mathcal{N}=2$ gauge multiplets, the gravitino supermultiplet is described by unconstrained analytic prepotentials $h^{++\\alpha}$ and $h^{+++}$ which contain a conformal gravitino in the Wess-Zumino gauge. The analytic prepotentials naturally come out from the study of $\\mathcal{N}=2$ supercurrents associated with hidden symmetries of $\\mathcal{N}=2$ vector-hypermultiplet system. We construct the co"},"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":"2412.14822","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-12-19T13:13:17Z","cross_cats_sorted":[],"title_canon_sha256":"15ff97dc7f3a2ad094dfb1eae350c071115c05f618edfc1ada0914503f678335","abstract_canon_sha256":"d20355fd783a397acc4f8eb324b44a4e873eb44ced10a958d10218928fc05f05"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T12:01:56.734941Z","signature_b64":"Y5sm+OJjn6v3nHSX08fQZtYB5MH8JVMMG+qSNnbeN2eqihBEF3lukJa1uU4L0Qs2vWr+SdxbJJ/ussBePMkbBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8880510e2611c5aeb387a10ff60f659f425902b47846b33fa650420701cfe1b8","last_reissued_at":"2026-07-05T12:01:56.734171Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T12:01:56.734171Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$\\mathcal{N}=2$ superconformal gravitino in harmonic superspace","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Evgeny Ivanov, Nikita Zaigraev","submitted_at":"2024-12-19T13:13:17Z","abstract_excerpt":"We present the harmonic superspace formulation of $\\mathcal{N}=2$ gravitino multiplet, the simplest $\\mathcal{N}=2$ half-integer spin gauge supermultiplet. It is shown that, quite similar to other $\\mathcal{N}=2$ gauge multiplets, the gravitino supermultiplet is described by unconstrained analytic prepotentials $h^{++\\alpha}$ and $h^{+++}$ which contain a conformal gravitino in the Wess-Zumino gauge. The analytic prepotentials naturally come out from the study of $\\mathcal{N}=2$ supercurrents associated with hidden symmetries of $\\mathcal{N}=2$ vector-hypermultiplet system. We construct the co"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2412.14822","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/2412.14822/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":"2412.14822","created_at":"2026-07-05T12:01:56.734257+00:00"},{"alias_kind":"arxiv_version","alias_value":"2412.14822v2","created_at":"2026-07-05T12:01:56.734257+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2412.14822","created_at":"2026-07-05T12:01:56.734257+00:00"},{"alias_kind":"pith_short_12","alias_value":"RCAFCDRGCHC2","created_at":"2026-07-05T12:01:56.734257+00:00"},{"alias_kind":"pith_short_16","alias_value":"RCAFCDRGCHC25M4H","created_at":"2026-07-05T12:01:56.734257+00:00"},{"alias_kind":"pith_short_8","alias_value":"RCAFCDRG","created_at":"2026-07-05T12:01:56.734257+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.25063","citing_title":"Supersymmetry at BLTP: Recent Progress in Two Directions","ref_index":27,"is_internal_anchor":false},{"citing_arxiv_id":"2605.27206","citing_title":"Structure of $\\mathcal{N} = 2$ superfield higher-spin abelian cubic interactions","ref_index":96,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RCAFCDRGCHC25M4HUEH7MD3FT5","json":"https://pith.science/pith/RCAFCDRGCHC25M4HUEH7MD3FT5.json","graph_json":"https://pith.science/api/pith-number/RCAFCDRGCHC25M4HUEH7MD3FT5/graph.json","events_json":"https://pith.science/api/pith-number/RCAFCDRGCHC25M4HUEH7MD3FT5/events.json","paper":"https://pith.science/paper/RCAFCDRG"},"agent_actions":{"view_html":"https://pith.science/pith/RCAFCDRGCHC25M4HUEH7MD3FT5","download_json":"https://pith.science/pith/RCAFCDRGCHC25M4HUEH7MD3FT5.json","view_paper":"https://pith.science/paper/RCAFCDRG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2412.14822&json=true","fetch_graph":"https://pith.science/api/pith-number/RCAFCDRGCHC25M4HUEH7MD3FT5/graph.json","fetch_events":"https://pith.science/api/pith-number/RCAFCDRGCHC25M4HUEH7MD3FT5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RCAFCDRGCHC25M4HUEH7MD3FT5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RCAFCDRGCHC25M4HUEH7MD3FT5/action/storage_attestation","attest_author":"https://pith.science/pith/RCAFCDRGCHC25M4HUEH7MD3FT5/action/author_attestation","sign_citation":"https://pith.science/pith/RCAFCDRGCHC25M4HUEH7MD3FT5/action/citation_signature","submit_replication":"https://pith.science/pith/RCAFCDRGCHC25M4HUEH7MD3FT5/action/replication_record"}},"created_at":"2026-07-05T12:01:56.734257+00:00","updated_at":"2026-07-05T12:01:56.734257+00:00"}