{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:MQQVIOQ6WOKP3FLWIPNR6F2ZIX","short_pith_number":"pith:MQQVIOQ6","schema_version":"1.0","canonical_sha256":"6421543a1eb394fd957643db1f175945fa394a722fd5c956a955890976da5da1","source":{"kind":"arxiv","id":"2603.27567","version":2},"attestation_state":"computed","paper":{"title":"One-loop finiteness in higher-derivative $6D$, ${\\cal N}=(1,0)$ super Yang-Mills -- hypermultiplet system","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A.S.Budekhina, E.A.Ivanov, I.L.Buchbinder, K.V.Stepanyantz","submitted_at":"2026-03-29T08:00:40Z","abstract_excerpt":"We employ the harmonic superspace methods to study a six-dimensional $\\mathcal{N}=(1,0)$ supersymmetric gauge theory with higher derivatives coupled to a hypermultiplet in the adjoint representation. By introducing a novel non-minimal interaction between the gauge multiplet and the hypermultiplet, we demonstrate that the one-loop divergences in gauge superfield sector, which are present in the conventional formulation, are canceled. The resulting theory is off-shell one-loop finite in this sector, while preserving the gauge invariance and $\\mathcal{N}=(1,0)$ supersymmetry. The cancelation mech"},"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":"2603.27567","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-03-29T08:00:40Z","cross_cats_sorted":[],"title_canon_sha256":"3213575b718257e65aede75daf53b1015b7f82b9e9046e8a30efdfccb98eb861","abstract_canon_sha256":"3ade1d35fa271fa067ff3cb5bb001981e68b25ca878bec37ed6fcd45528dcd69"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-20T01:05:11.984213Z","signature_b64":"/QI1eO5/jIQMaWIangit+0S4MaMmn1G4u2IWmCudvLEdRYJo/6KT7pXcYbQMvyqpMy+2hJe6gQBbiR3xwQoFDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6421543a1eb394fd957643db1f175945fa394a722fd5c956a955890976da5da1","last_reissued_at":"2026-05-20T01:05:11.983549Z","signature_status":"signed_v1","first_computed_at":"2026-05-20T01:05:11.983549Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"One-loop finiteness in higher-derivative $6D$, ${\\cal N}=(1,0)$ super Yang-Mills -- hypermultiplet system","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A.S.Budekhina, E.A.Ivanov, I.L.Buchbinder, K.V.Stepanyantz","submitted_at":"2026-03-29T08:00:40Z","abstract_excerpt":"We employ the harmonic superspace methods to study a six-dimensional $\\mathcal{N}=(1,0)$ supersymmetric gauge theory with higher derivatives coupled to a hypermultiplet in the adjoint representation. By introducing a novel non-minimal interaction between the gauge multiplet and the hypermultiplet, we demonstrate that the one-loop divergences in gauge superfield sector, which are present in the conventional formulation, are canceled. The resulting theory is off-shell one-loop finite in this sector, while preserving the gauge invariance and $\\mathcal{N}=(1,0)$ supersymmetry. The cancelation mech"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2603.27567","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/2603.27567/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":"2603.27567","created_at":"2026-05-20T01:05:11.983656+00:00"},{"alias_kind":"arxiv_version","alias_value":"2603.27567v2","created_at":"2026-05-20T01:05:11.983656+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2603.27567","created_at":"2026-05-20T01:05:11.983656+00:00"},{"alias_kind":"pith_short_12","alias_value":"MQQVIOQ6WOKP","created_at":"2026-05-20T01:05:11.983656+00:00"},{"alias_kind":"pith_short_16","alias_value":"MQQVIOQ6WOKP3FLW","created_at":"2026-05-20T01:05:11.983656+00:00"},{"alias_kind":"pith_short_8","alias_value":"MQQVIOQ6","created_at":"2026-05-20T01:05:11.983656+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.04378","citing_title":"Emergence of conformal properties in Finite Grand Unified Theories via reduction of couplings","ref_index":86,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MQQVIOQ6WOKP3FLWIPNR6F2ZIX","json":"https://pith.science/pith/MQQVIOQ6WOKP3FLWIPNR6F2ZIX.json","graph_json":"https://pith.science/api/pith-number/MQQVIOQ6WOKP3FLWIPNR6F2ZIX/graph.json","events_json":"https://pith.science/api/pith-number/MQQVIOQ6WOKP3FLWIPNR6F2ZIX/events.json","paper":"https://pith.science/paper/MQQVIOQ6"},"agent_actions":{"view_html":"https://pith.science/pith/MQQVIOQ6WOKP3FLWIPNR6F2ZIX","download_json":"https://pith.science/pith/MQQVIOQ6WOKP3FLWIPNR6F2ZIX.json","view_paper":"https://pith.science/paper/MQQVIOQ6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2603.27567&json=true","fetch_graph":"https://pith.science/api/pith-number/MQQVIOQ6WOKP3FLWIPNR6F2ZIX/graph.json","fetch_events":"https://pith.science/api/pith-number/MQQVIOQ6WOKP3FLWIPNR6F2ZIX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MQQVIOQ6WOKP3FLWIPNR6F2ZIX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MQQVIOQ6WOKP3FLWIPNR6F2ZIX/action/storage_attestation","attest_author":"https://pith.science/pith/MQQVIOQ6WOKP3FLWIPNR6F2ZIX/action/author_attestation","sign_citation":"https://pith.science/pith/MQQVIOQ6WOKP3FLWIPNR6F2ZIX/action/citation_signature","submit_replication":"https://pith.science/pith/MQQVIOQ6WOKP3FLWIPNR6F2ZIX/action/replication_record"}},"created_at":"2026-05-20T01:05:11.983656+00:00","updated_at":"2026-05-20T01:05:11.983656+00:00"}