{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:LZOWH7TLS52Q7UREVHTHE22PKU","short_pith_number":"pith:LZOWH7TL","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"},"canonical_sha256":"5e5d63fe6b97750fd224a9e6726b4f552da1b0fc798b7843b2c13678632aff61","source":{"kind":"arxiv","id":"1611.04804","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1611.04804","created_at":"2026-05-18T00:38:09Z"},{"alias_kind":"arxiv_version","alias_value":"1611.04804v3","created_at":"2026-05-18T00:38:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.04804","created_at":"2026-05-18T00:38:09Z"},{"alias_kind":"pith_short_12","alias_value":"LZOWH7TLS52Q","created_at":"2026-05-18T12:30:29Z"},{"alias_kind":"pith_short_16","alias_value":"LZOWH7TLS52Q7URE","created_at":"2026-05-18T12:30:29Z"},{"alias_kind":"pith_short_8","alias_value":"LZOWH7TL","created_at":"2026-05-18T12:30:29Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:LZOWH7TLS52Q7UREVHTHE22PKU","target":"record","payload":{"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"},"canonical_sha256":"5e5d63fe6b97750fd224a9e6726b4f552da1b0fc798b7843b2c13678632aff61","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"},"source_kind":"arxiv","source_id":"1611.04804","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:38:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dEvsWLINbH8OPqhR3nAJRyTzA2x3Vp+JhzNNy67Bdr9wXVvoTmETsk+xkGrr4S9zKh7qJjGdiKyh6zXh+XUbCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T16:55:58.131046Z"},"content_sha256":"5e91eef62fdc8ad877ca8d0cc2489114ee931aedbd196c38903159c43a2ebd82","schema_version":"1.0","event_id":"sha256:5e91eef62fdc8ad877ca8d0cc2489114ee931aedbd196c38903159c43a2ebd82"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:LZOWH7TLS52Q7UREVHTHE22PKU","target":"graph","payload":{"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:38:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ADrNk+lxjAGsA+IYwjO26bKQZIkHw4ncYoX8kpSYybRzQJ6EbuqxGl1Z+7Nd1Oxvqj3aEa45Z0KcuDgi9whNDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T16:55:58.131492Z"},"content_sha256":"b1caf9b2783cbce7fb332db5f516f3e1d76e1b8a475e8b539437299e63b4d86c","schema_version":"1.0","event_id":"sha256:b1caf9b2783cbce7fb332db5f516f3e1d76e1b8a475e8b539437299e63b4d86c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LZOWH7TLS52Q7UREVHTHE22PKU/bundle.json","state_url":"https://pith.science/pith/LZOWH7TLS52Q7UREVHTHE22PKU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LZOWH7TLS52Q7UREVHTHE22PKU/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-26T16:55:58Z","links":{"resolver":"https://pith.science/pith/LZOWH7TLS52Q7UREVHTHE22PKU","bundle":"https://pith.science/pith/LZOWH7TLS52Q7UREVHTHE22PKU/bundle.json","state":"https://pith.science/pith/LZOWH7TLS52Q7UREVHTHE22PKU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LZOWH7TLS52Q7UREVHTHE22PKU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:LZOWH7TLS52Q7UREVHTHE22PKU","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"93870c943fd97b2d32485fd36aaef352748cac502c18d15ee93dc8a5d215850e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-11-15T12:24:10Z","title_canon_sha256":"379eb47974bdd242642b35fea2ab42ef50e1509381b53efc04d7762689ce5a37"},"schema_version":"1.0","source":{"id":"1611.04804","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1611.04804","created_at":"2026-05-18T00:38:09Z"},{"alias_kind":"arxiv_version","alias_value":"1611.04804v3","created_at":"2026-05-18T00:38:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.04804","created_at":"2026-05-18T00:38:09Z"},{"alias_kind":"pith_short_12","alias_value":"LZOWH7TLS52Q","created_at":"2026-05-18T12:30:29Z"},{"alias_kind":"pith_short_16","alias_value":"LZOWH7TLS52Q7URE","created_at":"2026-05-18T12:30:29Z"},{"alias_kind":"pith_short_8","alias_value":"LZOWH7TL","created_at":"2026-05-18T12:30:29Z"}],"graph_snapshots":[{"event_id":"sha256:b1caf9b2783cbce7fb332db5f516f3e1d76e1b8a475e8b539437299e63b4d86c","target":"graph","created_at":"2026-05-18T00:38:09Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"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","authors_text":"Edi Gava, K.S. Narain, Nouman Muteeb, V. I. Giraldo-Rivera","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-11-15T12:24:10Z","title":"N=2 gauge theories on the hemisphere $HS^4$"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.04804","kind":"arxiv","version":3},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:5e91eef62fdc8ad877ca8d0cc2489114ee931aedbd196c38903159c43a2ebd82","target":"record","created_at":"2026-05-18T00:38:09Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"93870c943fd97b2d32485fd36aaef352748cac502c18d15ee93dc8a5d215850e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-11-15T12:24:10Z","title_canon_sha256":"379eb47974bdd242642b35fea2ab42ef50e1509381b53efc04d7762689ce5a37"},"schema_version":"1.0","source":{"id":"1611.04804","kind":"arxiv","version":3}},"canonical_sha256":"5e5d63fe6b97750fd224a9e6726b4f552da1b0fc798b7843b2c13678632aff61","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5e5d63fe6b97750fd224a9e6726b4f552da1b0fc798b7843b2c13678632aff61","first_computed_at":"2026-05-18T00:38:09.213006Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:38:09.213006Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"o1ujfPLkPEldq1JHJFDwoPqOTkQWIjUUwE6y8BsROHadIr4KMNlT9Ma+jdu18YJ03jh5NBsdFRTEJxLCB+8eDw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:38:09.213485Z","signed_message":"canonical_sha256_bytes"},"source_id":"1611.04804","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5e91eef62fdc8ad877ca8d0cc2489114ee931aedbd196c38903159c43a2ebd82","sha256:b1caf9b2783cbce7fb332db5f516f3e1d76e1b8a475e8b539437299e63b4d86c"],"state_sha256":"c28f35c61169617b92695c153b0ec1f4d6b8ef91308ec710d0cacd5689217642"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uYrS+b6GSDIhyyjNHvLL7v6OsaNLvkuZcpOff3O8V1QZvfmvUT6KpI8GTHdl7jrxRgeHmW6iXXO0fvonUdYVAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T16:55:58.134478Z","bundle_sha256":"95d42659613d5b0cf506173c20062902e6a42cbc0fb16b65ba049a833cfe9591"}}