{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1998:E3TVSSYASOUSPTWIRJJBRBM3CQ","short_pith_number":"pith:E3TVSSYA","canonical_record":{"source":{"id":"hep-th/9808075","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1998-08-12T22:02:34Z","cross_cats_sorted":[],"title_canon_sha256":"a21971a894e6219272dc2e1a3a3dd0d639a2e757226fc828cf72ab29612e0f63","abstract_canon_sha256":"87bba1516e5e4a8421d832cee7b54e2708cfbbd75b01d8bd15b5f1d744029274"},"schema_version":"1.0"},"canonical_sha256":"26e7594b0093a927cec88a5218859b142b29b5944a032da58089851e9fcd10ff","source":{"kind":"arxiv","id":"hep-th/9808075","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9808075","created_at":"2026-05-18T01:08:01Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9808075v2","created_at":"2026-05-18T01:08:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9808075","created_at":"2026-05-18T01:08:01Z"},{"alias_kind":"pith_short_12","alias_value":"E3TVSSYASOUS","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_16","alias_value":"E3TVSSYASOUSPTWI","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_8","alias_value":"E3TVSSYA","created_at":"2026-05-18T12:25:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1998:E3TVSSYASOUSPTWIRJJBRBM3CQ","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/9808075","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1998-08-12T22:02:34Z","cross_cats_sorted":[],"title_canon_sha256":"a21971a894e6219272dc2e1a3a3dd0d639a2e757226fc828cf72ab29612e0f63","abstract_canon_sha256":"87bba1516e5e4a8421d832cee7b54e2708cfbbd75b01d8bd15b5f1d744029274"},"schema_version":"1.0"},"canonical_sha256":"26e7594b0093a927cec88a5218859b142b29b5944a032da58089851e9fcd10ff","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:08:01.528411Z","signature_b64":"w3d+H+Q37Zt/BGRYblGOvsjtcv70EAWFtBR9E05J1bG9lmXZ8S38RV8fVNiQgxq8nbnw5r/uskOrnDMieE5KCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"26e7594b0093a927cec88a5218859b142b29b5944a032da58089851e9fcd10ff","last_reissued_at":"2026-05-18T01:08:01.527895Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:08:01.527895Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/9808075","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:08:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ycrHIOVPZs3KCYPbsBs54DN84ffQ2q5uGtuXiDUM42A/AuJpC/HSH/nrFlEelt8+p7FPlOXHdKwA22jA9GK8DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T04:24:08.346475Z"},"content_sha256":"83d790aca3e50cd6a1d9de22139106a91eeb2e7d964e884cf4dee11fcc28ec1d","schema_version":"1.0","event_id":"sha256:83d790aca3e50cd6a1d9de22139106a91eeb2e7d964e884cf4dee11fcc28ec1d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1998:E3TVSSYASOUSPTWIRJJBRBM3CQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Baryons and Domain Walls in an N = 1 Superconformal Gauge Theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Igor R. Klebanov, Steven S. Gubser","submitted_at":"1998-08-12T22:02:34Z","abstract_excerpt":"Coincident D3-branes placed at a conical singularity are related to string theory on $AdS_5\\times X_5$, for a suitable five-dimensional Einstein manifold $X_5$. For the example of the conifold, which leads to $X_5=T^{1,1}=(SU(2)\\times SU(2))/U(1)$, the infrared limit of the theory on $N$ D3-branes was constructed recently. This is ${\\cal N}=1$ supersymmetric $SU(N)\\times SU(N)$ gauge theory coupled to four bifundamental chiral superfields and supplemented by a quartic superpotential which becomes marginal in the infrared. In this paper we consider D3-branes wrapped over the 3-cycles of $T^{1,1"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9808075","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":""},"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":"2026-05-18T01:08:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yhNscVkC6mPplitOS0TIYCiT+7VMKcX3ToAQl0lil+jxwwBWYCAb4XsLRAiYoOnkj4YayC7Rsm1EdxkK5WUuAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T04:24:08.347109Z"},"content_sha256":"68265181f412d7a3a76946ae9d3c466b6636e198eac21c46d89602e20906c94e","schema_version":"1.0","event_id":"sha256:68265181f412d7a3a76946ae9d3c466b6636e198eac21c46d89602e20906c94e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/E3TVSSYASOUSPTWIRJJBRBM3CQ/bundle.json","state_url":"https://pith.science/pith/E3TVSSYASOUSPTWIRJJBRBM3CQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/E3TVSSYASOUSPTWIRJJBRBM3CQ/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":"2026-05-27T04:24:08Z","links":{"resolver":"https://pith.science/pith/E3TVSSYASOUSPTWIRJJBRBM3CQ","bundle":"https://pith.science/pith/E3TVSSYASOUSPTWIRJJBRBM3CQ/bundle.json","state":"https://pith.science/pith/E3TVSSYASOUSPTWIRJJBRBM3CQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/E3TVSSYASOUSPTWIRJJBRBM3CQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1998:E3TVSSYASOUSPTWIRJJBRBM3CQ","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":"87bba1516e5e4a8421d832cee7b54e2708cfbbd75b01d8bd15b5f1d744029274","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1998-08-12T22:02:34Z","title_canon_sha256":"a21971a894e6219272dc2e1a3a3dd0d639a2e757226fc828cf72ab29612e0f63"},"schema_version":"1.0","source":{"id":"hep-th/9808075","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9808075","created_at":"2026-05-18T01:08:01Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9808075v2","created_at":"2026-05-18T01:08:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9808075","created_at":"2026-05-18T01:08:01Z"},{"alias_kind":"pith_short_12","alias_value":"E3TVSSYASOUS","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_16","alias_value":"E3TVSSYASOUSPTWI","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_8","alias_value":"E3TVSSYA","created_at":"2026-05-18T12:25:49Z"}],"graph_snapshots":[{"event_id":"sha256:68265181f412d7a3a76946ae9d3c466b6636e198eac21c46d89602e20906c94e","target":"graph","created_at":"2026-05-18T01:08:01Z","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":"Coincident D3-branes placed at a conical singularity are related to string theory on $AdS_5\\times X_5$, for a suitable five-dimensional Einstein manifold $X_5$. For the example of the conifold, which leads to $X_5=T^{1,1}=(SU(2)\\times SU(2))/U(1)$, the infrared limit of the theory on $N$ D3-branes was constructed recently. This is ${\\cal N}=1$ supersymmetric $SU(N)\\times SU(N)$ gauge theory coupled to four bifundamental chiral superfields and supplemented by a quartic superpotential which becomes marginal in the infrared. In this paper we consider D3-branes wrapped over the 3-cycles of $T^{1,1","authors_text":"Igor R. Klebanov, Steven S. Gubser","cross_cats":[],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"1998-08-12T22:02:34Z","title":"Baryons and Domain Walls in an N = 1 Superconformal Gauge Theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9808075","kind":"arxiv","version":2},"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":"sha256:83d790aca3e50cd6a1d9de22139106a91eeb2e7d964e884cf4dee11fcc28ec1d","target":"record","created_at":"2026-05-18T01:08:01Z","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":"87bba1516e5e4a8421d832cee7b54e2708cfbbd75b01d8bd15b5f1d744029274","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1998-08-12T22:02:34Z","title_canon_sha256":"a21971a894e6219272dc2e1a3a3dd0d639a2e757226fc828cf72ab29612e0f63"},"schema_version":"1.0","source":{"id":"hep-th/9808075","kind":"arxiv","version":2}},"canonical_sha256":"26e7594b0093a927cec88a5218859b142b29b5944a032da58089851e9fcd10ff","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"26e7594b0093a927cec88a5218859b142b29b5944a032da58089851e9fcd10ff","first_computed_at":"2026-05-18T01:08:01.527895Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:08:01.527895Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"w3d+H+Q37Zt/BGRYblGOvsjtcv70EAWFtBR9E05J1bG9lmXZ8S38RV8fVNiQgxq8nbnw5r/uskOrnDMieE5KCw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:08:01.528411Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/9808075","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:83d790aca3e50cd6a1d9de22139106a91eeb2e7d964e884cf4dee11fcc28ec1d","sha256:68265181f412d7a3a76946ae9d3c466b6636e198eac21c46d89602e20906c94e"],"state_sha256":"c6cc89cda4892ef6156d0c9c27a4196f06b592e3984fabd81d4c4090b131c07e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MwGF76YGSVZ1JxUZUOzFfiZraBsN5/tOz2NU9ydZlxraRZC+fZbaE6ov8eXdAx+GFztkoiBU8EerCjp6nHJRDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T04:24:08.350350Z","bundle_sha256":"c82de13bfa2a22121e38636b35282a962c86ae77d47f78865c875c54a6e96389"}}