{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:LEXOQXFPLFHROBVN3CM75OOUME","short_pith_number":"pith:LEXOQXFP","schema_version":"1.0","canonical_sha256":"592ee85caf594f1706add899feb9d4610910e0a575d0de342fe02e1a7faf94d2","source":{"kind":"arxiv","id":"1612.07991","version":2},"attestation_state":"computed","paper":{"title":"Circular Wilson loops in defect Conformal Field Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Diego H. Correa, Jeremias Aguilera-Damia, Victor I. Giraldo-Rivera","submitted_at":"2016-12-23T14:58:30Z","abstract_excerpt":"We study a D3-D5 system dual to a conformal field theory with a codimension-one defect that separates regions where the ranks of the gauge groups differ by $k$. With the help of this additional parameter, as observed by Nagasaki, Tanida and Yamaguchi, one can define a double scaling limit in which the quantum corrections are organized in powers of $\\lambda/k^2$, which should allow to extrapolate results between weak and strong coupling regimes. In particular we consider a radius $R$ circular Wilson loop placed at a distance $L$, whose internal space orientation is given by an angle $\\chi$. We "},"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":"1612.07991","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-12-23T14:58:30Z","cross_cats_sorted":[],"title_canon_sha256":"a3f38c0cfef01b950081021f4469e7fe9eda199b5722fad5d818d498543f9c70","abstract_canon_sha256":"c0a7573eb9a30d4e06d83bb5dfa09a5a4a2c5af02f19dd0b300850bd68588530"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:47:05.043008Z","signature_b64":"xXbpfoDv1aCdteY7OmPAO55cxQaGRyH0ZZYmIiaSu7uQteWYBAnWYtgQNaaJlKqlB4+I8FUIIMGPF97JVjBxDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"592ee85caf594f1706add899feb9d4610910e0a575d0de342fe02e1a7faf94d2","last_reissued_at":"2026-05-18T00:47:05.042461Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:47:05.042461Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Circular Wilson loops in defect Conformal Field Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Diego H. Correa, Jeremias Aguilera-Damia, Victor I. Giraldo-Rivera","submitted_at":"2016-12-23T14:58:30Z","abstract_excerpt":"We study a D3-D5 system dual to a conformal field theory with a codimension-one defect that separates regions where the ranks of the gauge groups differ by $k$. With the help of this additional parameter, as observed by Nagasaki, Tanida and Yamaguchi, one can define a double scaling limit in which the quantum corrections are organized in powers of $\\lambda/k^2$, which should allow to extrapolate results between weak and strong coupling regimes. In particular we consider a radius $R$ circular Wilson loop placed at a distance $L$, whose internal space orientation is given by an angle $\\chi$. We "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1612.07991","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1612.07991","created_at":"2026-05-18T00:47:05.042539+00:00"},{"alias_kind":"arxiv_version","alias_value":"1612.07991v2","created_at":"2026-05-18T00:47:05.042539+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1612.07991","created_at":"2026-05-18T00:47:05.042539+00:00"},{"alias_kind":"pith_short_12","alias_value":"LEXOQXFPLFHR","created_at":"2026-05-18T12:30:29.479603+00:00"},{"alias_kind":"pith_short_16","alias_value":"LEXOQXFPLFHROBVN","created_at":"2026-05-18T12:30:29.479603+00:00"},{"alias_kind":"pith_short_8","alias_value":"LEXOQXFP","created_at":"2026-05-18T12:30:29.479603+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2512.05514","citing_title":"Wilson loops on the Coulomb branch of $N=4$ super-Yang-Mills","ref_index":5,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LEXOQXFPLFHROBVN3CM75OOUME","json":"https://pith.science/pith/LEXOQXFPLFHROBVN3CM75OOUME.json","graph_json":"https://pith.science/api/pith-number/LEXOQXFPLFHROBVN3CM75OOUME/graph.json","events_json":"https://pith.science/api/pith-number/LEXOQXFPLFHROBVN3CM75OOUME/events.json","paper":"https://pith.science/paper/LEXOQXFP"},"agent_actions":{"view_html":"https://pith.science/pith/LEXOQXFPLFHROBVN3CM75OOUME","download_json":"https://pith.science/pith/LEXOQXFPLFHROBVN3CM75OOUME.json","view_paper":"https://pith.science/paper/LEXOQXFP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1612.07991&json=true","fetch_graph":"https://pith.science/api/pith-number/LEXOQXFPLFHROBVN3CM75OOUME/graph.json","fetch_events":"https://pith.science/api/pith-number/LEXOQXFPLFHROBVN3CM75OOUME/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LEXOQXFPLFHROBVN3CM75OOUME/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LEXOQXFPLFHROBVN3CM75OOUME/action/storage_attestation","attest_author":"https://pith.science/pith/LEXOQXFPLFHROBVN3CM75OOUME/action/author_attestation","sign_citation":"https://pith.science/pith/LEXOQXFPLFHROBVN3CM75OOUME/action/citation_signature","submit_replication":"https://pith.science/pith/LEXOQXFPLFHROBVN3CM75OOUME/action/replication_record"}},"created_at":"2026-05-18T00:47:05.042539+00:00","updated_at":"2026-05-18T00:47:05.042539+00:00"}