{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:Y5SKFLDTHYV7VYZG6ZN6GILLUU","short_pith_number":"pith:Y5SKFLDT","canonical_record":{"source":{"id":"1406.5501","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-06-20T19:52:05Z","cross_cats_sorted":[],"title_canon_sha256":"0610d4bd32e621805096c444f7f879ed2d80381acda3eede99ade80681832aa5","abstract_canon_sha256":"dc9bf3c49135231c997f81023fc70ef2daadea6cd5321548fea109d206454e1d"},"schema_version":"1.0"},"canonical_sha256":"c764a2ac733e2bfae326f65be3216ba52f3492e334c277aa368da66442ae24e7","source":{"kind":"arxiv","id":"1406.5501","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1406.5501","created_at":"2026-05-18T02:39:23Z"},{"alias_kind":"arxiv_version","alias_value":"1406.5501v1","created_at":"2026-05-18T02:39:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1406.5501","created_at":"2026-05-18T02:39:23Z"},{"alias_kind":"pith_short_12","alias_value":"Y5SKFLDTHYV7","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_16","alias_value":"Y5SKFLDTHYV7VYZG","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_8","alias_value":"Y5SKFLDT","created_at":"2026-05-18T12:28:57Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:Y5SKFLDTHYV7VYZG6ZN6GILLUU","target":"record","payload":{"canonical_record":{"source":{"id":"1406.5501","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-06-20T19:52:05Z","cross_cats_sorted":[],"title_canon_sha256":"0610d4bd32e621805096c444f7f879ed2d80381acda3eede99ade80681832aa5","abstract_canon_sha256":"dc9bf3c49135231c997f81023fc70ef2daadea6cd5321548fea109d206454e1d"},"schema_version":"1.0"},"canonical_sha256":"c764a2ac733e2bfae326f65be3216ba52f3492e334c277aa368da66442ae24e7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:39:23.627624Z","signature_b64":"2R7EZSBghYlLQoEpQfhku+yygB6y4m+64JMavJmAVuLGSnRMxQ17/+38jL/Hgciiw4pRF0NRvVl5EbQdtA2vDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c764a2ac733e2bfae326f65be3216ba52f3492e334c277aa368da66442ae24e7","last_reissued_at":"2026-05-18T02:39:23.627255Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:39:23.627255Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1406.5501","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:39:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GUtxuRG6iGxhX+tDlpbSK8yg6QHyZ8Ta7EQUnGSqYWBpDYKDvU1fL78rYUoS9wOWyneGWxS06C9BRpH4GdxpDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T09:15:28.118738Z"},"content_sha256":"49e3e677420350f956d8b2760be6a7614350d8ee1c540406126e8b21b647f8d8","schema_version":"1.0","event_id":"sha256:49e3e677420350f956d8b2760be6a7614350d8ee1c540406126e8b21b647f8d8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:Y5SKFLDTHYV7VYZG6ZN6GILLUU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Boundaries and Defects of N=4 SYM with 4 Supercharges, Part II: Brane Constructions and 3d N=2 Field Theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Akikazu Hashimoto, Masahito Yamazaki, Peter Ouyang","submitted_at":"2014-06-20T19:52:05Z","abstract_excerpt":"We study the vacuum moduli spaces of 3d N=2 supersymmetric quantum field theories by applying the formalism developed in our previous paper arXiv:1404.5527. The 3d theories can be realized by branes in type IIB string theory, which in a decoupling limit reduce to 4d N=4 super-Yang-Mills theory on an interval with BPS defects inserted. The moduli space of a given 3d theory is obtained by solving a generalization of Nahm's equations with appropriate boundary/junction conditions, along with help from the S-duality of type IIB string theory. Our classical computations reproduce many known results "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1406.5501","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":""},"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":"2026-05-18T02:39:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/6QuegAxDA4F0hSp1zCVt139HDehDWyknY8BYYO0C9CX8vBc9nBT4tYxMN2iFnd/hU9aVat6m770feIqy5ndBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T09:15:28.119478Z"},"content_sha256":"d35d4f53c99ed988805c25be0348be375ecbfdefd031ce56bc15ca4759004a6c","schema_version":"1.0","event_id":"sha256:d35d4f53c99ed988805c25be0348be375ecbfdefd031ce56bc15ca4759004a6c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/Y5SKFLDTHYV7VYZG6ZN6GILLUU/bundle.json","state_url":"https://pith.science/pith/Y5SKFLDTHYV7VYZG6ZN6GILLUU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/Y5SKFLDTHYV7VYZG6ZN6GILLUU/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":"2026-06-09T09:15:28Z","links":{"resolver":"https://pith.science/pith/Y5SKFLDTHYV7VYZG6ZN6GILLUU","bundle":"https://pith.science/pith/Y5SKFLDTHYV7VYZG6ZN6GILLUU/bundle.json","state":"https://pith.science/pith/Y5SKFLDTHYV7VYZG6ZN6GILLUU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/Y5SKFLDTHYV7VYZG6ZN6GILLUU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:Y5SKFLDTHYV7VYZG6ZN6GILLUU","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":"dc9bf3c49135231c997f81023fc70ef2daadea6cd5321548fea109d206454e1d","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-06-20T19:52:05Z","title_canon_sha256":"0610d4bd32e621805096c444f7f879ed2d80381acda3eede99ade80681832aa5"},"schema_version":"1.0","source":{"id":"1406.5501","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1406.5501","created_at":"2026-05-18T02:39:23Z"},{"alias_kind":"arxiv_version","alias_value":"1406.5501v1","created_at":"2026-05-18T02:39:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1406.5501","created_at":"2026-05-18T02:39:23Z"},{"alias_kind":"pith_short_12","alias_value":"Y5SKFLDTHYV7","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_16","alias_value":"Y5SKFLDTHYV7VYZG","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_8","alias_value":"Y5SKFLDT","created_at":"2026-05-18T12:28:57Z"}],"graph_snapshots":[{"event_id":"sha256:d35d4f53c99ed988805c25be0348be375ecbfdefd031ce56bc15ca4759004a6c","target":"graph","created_at":"2026-05-18T02:39:23Z","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":"We study the vacuum moduli spaces of 3d N=2 supersymmetric quantum field theories by applying the formalism developed in our previous paper arXiv:1404.5527. The 3d theories can be realized by branes in type IIB string theory, which in a decoupling limit reduce to 4d N=4 super-Yang-Mills theory on an interval with BPS defects inserted. The moduli space of a given 3d theory is obtained by solving a generalization of Nahm's equations with appropriate boundary/junction conditions, along with help from the S-duality of type IIB string theory. Our classical computations reproduce many known results ","authors_text":"Akikazu Hashimoto, Masahito Yamazaki, Peter Ouyang","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-06-20T19:52:05Z","title":"Boundaries and Defects of N=4 SYM with 4 Supercharges, Part II: Brane Constructions and 3d N=2 Field Theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1406.5501","kind":"arxiv","version":1},"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":"sha256:49e3e677420350f956d8b2760be6a7614350d8ee1c540406126e8b21b647f8d8","target":"record","created_at":"2026-05-18T02:39:23Z","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":"dc9bf3c49135231c997f81023fc70ef2daadea6cd5321548fea109d206454e1d","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-06-20T19:52:05Z","title_canon_sha256":"0610d4bd32e621805096c444f7f879ed2d80381acda3eede99ade80681832aa5"},"schema_version":"1.0","source":{"id":"1406.5501","kind":"arxiv","version":1}},"canonical_sha256":"c764a2ac733e2bfae326f65be3216ba52f3492e334c277aa368da66442ae24e7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c764a2ac733e2bfae326f65be3216ba52f3492e334c277aa368da66442ae24e7","first_computed_at":"2026-05-18T02:39:23.627255Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:39:23.627255Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2R7EZSBghYlLQoEpQfhku+yygB6y4m+64JMavJmAVuLGSnRMxQ17/+38jL/Hgciiw4pRF0NRvVl5EbQdtA2vDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:39:23.627624Z","signed_message":"canonical_sha256_bytes"},"source_id":"1406.5501","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:49e3e677420350f956d8b2760be6a7614350d8ee1c540406126e8b21b647f8d8","sha256:d35d4f53c99ed988805c25be0348be375ecbfdefd031ce56bc15ca4759004a6c"],"state_sha256":"2cc5e6aa6704491f8ebb6137a68279debc9f31dfdcee3294fd910ff67be3eece"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SfrdiC8WejHwxdR7cEOt5o2blqgImm3hpPD2XSF4l0aDklUf35jTFHFrP+0YbFyMyhfOjqsOQjbxqEOQrW3uDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T09:15:28.123574Z","bundle_sha256":"e6b9fb8ee2df468e94ed9f297f8b4c672614733a7fa37225d00c51cbbfa270a7"}}