{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:LZOWH7TLS52Q7UREVHTHE22PKU","short_pith_number":"pith:LZOWH7TL","schema_version":"1.0","canonical_sha256":"5e5d63fe6b97750fd224a9e6726b4f552da1b0fc798b7843b2c13678632aff61","source":{"kind":"arxiv","id":"1611.04804","version":3},"attestation_state":"computed","paper":{"title":"N=2 gauge theories on the hemisphere $HS^4$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Edi Gava, K.S. Narain, Nouman Muteeb, V. I. Giraldo-Rivera","submitted_at":"2016-11-15T12:24:10Z","abstract_excerpt":"Using localization techniques, we compute the path integral of $N=2$ SUSY gauge theory coupled to matter on the hemisphere $HS^4$, with either Dirichlet or Neumann supersymmetric boundary conditions. The resulting quantities are wave-functions of the theory depending on the boundary data. The one-loop determinant are computed using $SO(4)$ harmonics basis. We solve kernel and co-kernel equations for the relevant differential operators arising from gauge and matter localizing actions. The second method utilizes full $SO(5)$ harmonics to reduce the computation to evaluating $Q_{SUSY}^2$ eigenval"},"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":"1611.04804","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-11-15T12:24:10Z","cross_cats_sorted":[],"title_canon_sha256":"379eb47974bdd242642b35fea2ab42ef50e1509381b53efc04d7762689ce5a37","abstract_canon_sha256":"93870c943fd97b2d32485fd36aaef352748cac502c18d15ee93dc8a5d215850e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:38:09.213485Z","signature_b64":"o1ujfPLkPEldq1JHJFDwoPqOTkQWIjUUwE6y8BsROHadIr4KMNlT9Ma+jdu18YJ03jh5NBsdFRTEJxLCB+8eDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5e5d63fe6b97750fd224a9e6726b4f552da1b0fc798b7843b2c13678632aff61","last_reissued_at":"2026-05-18T00:38:09.213006Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:38:09.213006Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"N=2 gauge theories on the hemisphere $HS^4$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Edi Gava, K.S. Narain, Nouman Muteeb, V. I. Giraldo-Rivera","submitted_at":"2016-11-15T12:24:10Z","abstract_excerpt":"Using localization techniques, we compute the path integral of $N=2$ SUSY gauge theory coupled to matter on the hemisphere $HS^4$, with either Dirichlet or Neumann supersymmetric boundary conditions. The resulting quantities are wave-functions of the theory depending on the boundary data. The one-loop determinant are computed using $SO(4)$ harmonics basis. We solve kernel and co-kernel equations for the relevant differential operators arising from gauge and matter localizing actions. The second method utilizes full $SO(5)$ harmonics to reduce the computation to evaluating $Q_{SUSY}^2$ eigenval"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.04804","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"1611.04804","created_at":"2026-05-18T00:38:09.213083+00:00"},{"alias_kind":"arxiv_version","alias_value":"1611.04804v3","created_at":"2026-05-18T00:38:09.213083+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.04804","created_at":"2026-05-18T00:38:09.213083+00:00"},{"alias_kind":"pith_short_12","alias_value":"LZOWH7TLS52Q","created_at":"2026-05-18T12:30:29.479603+00:00"},{"alias_kind":"pith_short_16","alias_value":"LZOWH7TLS52Q7URE","created_at":"2026-05-18T12:30:29.479603+00:00"},{"alias_kind":"pith_short_8","alias_value":"LZOWH7TL","created_at":"2026-05-18T12:30:29.479603+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/LZOWH7TLS52Q7UREVHTHE22PKU","json":"https://pith.science/pith/LZOWH7TLS52Q7UREVHTHE22PKU.json","graph_json":"https://pith.science/api/pith-number/LZOWH7TLS52Q7UREVHTHE22PKU/graph.json","events_json":"https://pith.science/api/pith-number/LZOWH7TLS52Q7UREVHTHE22PKU/events.json","paper":"https://pith.science/paper/LZOWH7TL"},"agent_actions":{"view_html":"https://pith.science/pith/LZOWH7TLS52Q7UREVHTHE22PKU","download_json":"https://pith.science/pith/LZOWH7TLS52Q7UREVHTHE22PKU.json","view_paper":"https://pith.science/paper/LZOWH7TL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1611.04804&json=true","fetch_graph":"https://pith.science/api/pith-number/LZOWH7TLS52Q7UREVHTHE22PKU/graph.json","fetch_events":"https://pith.science/api/pith-number/LZOWH7TLS52Q7UREVHTHE22PKU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LZOWH7TLS52Q7UREVHTHE22PKU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LZOWH7TLS52Q7UREVHTHE22PKU/action/storage_attestation","attest_author":"https://pith.science/pith/LZOWH7TLS52Q7UREVHTHE22PKU/action/author_attestation","sign_citation":"https://pith.science/pith/LZOWH7TLS52Q7UREVHTHE22PKU/action/citation_signature","submit_replication":"https://pith.science/pith/LZOWH7TLS52Q7UREVHTHE22PKU/action/replication_record"}},"created_at":"2026-05-18T00:38:09.213083+00:00","updated_at":"2026-05-18T00:38:09.213083+00:00"}