{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:HKFF26JOHJC2CHX6EYVBQ54ORV","short_pith_number":"pith:HKFF26JO","schema_version":"1.0","canonical_sha256":"3a8a5d792e3a45a11efe262a18778e8d51f9ae8edf60eb3e9f1b0ebdc70e12d8","source":{"kind":"arxiv","id":"hep-th/0207125","version":1},"attestation_state":"computed","paper":{"title":"BPS Branes From Baryons","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Chris E. Beasley","submitted_at":"2002-07-12T18:09:27Z","abstract_excerpt":"We elucidate the relationship between supersymmetric D3-branes and chiral baryonic operators in the AdS/CFT correspondence. For supersymmetric backgrounds of the form AdS_5 x H, we characterize via holomorphy a large family of supersymmetric D3-brane probes wrapped on H. We then quantize this classical family of probe solutions to obtain a BPS spectrum which describes D3-brane configurations on H. For the particular examples H = T^{1,1} and H = S^5, we match the BPS spectrum to the spectrum of chiral baryonic operators in the dual gauge theory."},"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":"hep-th/0207125","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2002-07-12T18:09:27Z","cross_cats_sorted":[],"title_canon_sha256":"646c398bd3161e64e8d8d772f9d3a7221b8f0c6137e36ab17862f342471612f7","abstract_canon_sha256":"d70d805d25391a2a8f1f090f31f0ef7f7b258d00562cab79ca25ec83089ba3c3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:34:49.814224Z","signature_b64":"z8naHeP70ZLSnhIDfPU6ntJ2TIHQqvHzotcIHaOr576qQFv4lFT7nc/5GDYvid/8SDsmXBu0dFhdKj9j24FSBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3a8a5d792e3a45a11efe262a18778e8d51f9ae8edf60eb3e9f1b0ebdc70e12d8","last_reissued_at":"2026-07-04T16:34:49.813881Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:34:49.813881Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"BPS Branes From Baryons","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Chris E. Beasley","submitted_at":"2002-07-12T18:09:27Z","abstract_excerpt":"We elucidate the relationship between supersymmetric D3-branes and chiral baryonic operators in the AdS/CFT correspondence. For supersymmetric backgrounds of the form AdS_5 x H, we characterize via holomorphy a large family of supersymmetric D3-brane probes wrapped on H. We then quantize this classical family of probe solutions to obtain a BPS spectrum which describes D3-brane configurations on H. For the particular examples H = T^{1,1} and H = S^5, we match the BPS spectrum to the spectrum of chiral baryonic operators in the dual gauge theory."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0207125","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/0207125/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":"hep-th/0207125","created_at":"2026-07-04T16:34:49.813941+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0207125v1","created_at":"2026-07-04T16:34:49.813941+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0207125","created_at":"2026-07-04T16:34:49.813941+00:00"},{"alias_kind":"pith_short_12","alias_value":"HKFF26JOHJC2","created_at":"2026-07-04T16:34:49.813941+00:00"},{"alias_kind":"pith_short_16","alias_value":"HKFF26JOHJC2CHX6","created_at":"2026-07-04T16:34:49.813941+00:00"},{"alias_kind":"pith_short_8","alias_value":"HKFF26JO","created_at":"2026-07-04T16:34:49.813941+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2605.16254","citing_title":"Fortuity and Complexity in a Simple Quark Model","ref_index":53,"is_internal_anchor":true},{"citing_arxiv_id":"2605.16254","citing_title":"Fortuity and Complexity in a Simple Quark Model","ref_index":41,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HKFF26JOHJC2CHX6EYVBQ54ORV","json":"https://pith.science/pith/HKFF26JOHJC2CHX6EYVBQ54ORV.json","graph_json":"https://pith.science/api/pith-number/HKFF26JOHJC2CHX6EYVBQ54ORV/graph.json","events_json":"https://pith.science/api/pith-number/HKFF26JOHJC2CHX6EYVBQ54ORV/events.json","paper":"https://pith.science/paper/HKFF26JO"},"agent_actions":{"view_html":"https://pith.science/pith/HKFF26JOHJC2CHX6EYVBQ54ORV","download_json":"https://pith.science/pith/HKFF26JOHJC2CHX6EYVBQ54ORV.json","view_paper":"https://pith.science/paper/HKFF26JO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0207125&json=true","fetch_graph":"https://pith.science/api/pith-number/HKFF26JOHJC2CHX6EYVBQ54ORV/graph.json","fetch_events":"https://pith.science/api/pith-number/HKFF26JOHJC2CHX6EYVBQ54ORV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HKFF26JOHJC2CHX6EYVBQ54ORV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HKFF26JOHJC2CHX6EYVBQ54ORV/action/storage_attestation","attest_author":"https://pith.science/pith/HKFF26JOHJC2CHX6EYVBQ54ORV/action/author_attestation","sign_citation":"https://pith.science/pith/HKFF26JOHJC2CHX6EYVBQ54ORV/action/citation_signature","submit_replication":"https://pith.science/pith/HKFF26JOHJC2CHX6EYVBQ54ORV/action/replication_record"}},"created_at":"2026-07-04T16:34:49.813941+00:00","updated_at":"2026-07-04T16:34:49.813941+00:00"}