{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:WAVYVJAT52MZRCUHJRS5NQJ2XY","short_pith_number":"pith:WAVYVJAT","schema_version":"1.0","canonical_sha256":"b02b8aa413ee99988a874c65d6c13abe09a23b89750ce68b88a84a649a8d412e","source":{"kind":"arxiv","id":"1911.05082","version":3},"attestation_state":"computed","paper":{"title":"Superconformal surfaces in four dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Lorenzo Bianchi, Madalena Lemos","submitted_at":"2019-11-12T19:00:02Z","abstract_excerpt":"We study the constraints of superconformal symmetry on codimension two defects in four-dimensional superconformal field theories. We show that the one-point function of the stress tensor and the two-point function of the displacement operator are related, and we discuss the consequences of this relation for the Weyl anomaly coefficients as well as in a few examples, including the supersymmetric R\\'enyi entropy. Imposing consistency with existing results, we propose a general relation that could hold for sufficiently supersymmetric defects of arbitrary dimension and codimension. Turning to $\\ma"},"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":"1911.05082","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-11-12T19:00:02Z","cross_cats_sorted":[],"title_canon_sha256":"e78092eb9ec23ed12688a80b98fe32e4dfaf13794a8d3f522137660ba1c5f56d","abstract_canon_sha256":"a0a434070efdaa5b4873c6f551e9c2ffb6c4e2ae244ee22cab8b17fa9a7f434b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:16:34.017304Z","signature_b64":"7BDk3GFPMKnM1RiAUliMTEVArVS1+mxpUVDogw8t0/Bjzx6FU9BICeImJasaiSHVVsw2QGXGrZ0W4Fve7PZfBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b02b8aa413ee99988a874c65d6c13abe09a23b89750ce68b88a84a649a8d412e","last_reissued_at":"2026-07-05T04:16:34.016846Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:16:34.016846Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Superconformal surfaces in four dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Lorenzo Bianchi, Madalena Lemos","submitted_at":"2019-11-12T19:00:02Z","abstract_excerpt":"We study the constraints of superconformal symmetry on codimension two defects in four-dimensional superconformal field theories. We show that the one-point function of the stress tensor and the two-point function of the displacement operator are related, and we discuss the consequences of this relation for the Weyl anomaly coefficients as well as in a few examples, including the supersymmetric R\\'enyi entropy. Imposing consistency with existing results, we propose a general relation that could hold for sufficiently supersymmetric defects of arbitrary dimension and codimension. Turning to $\\ma"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1911.05082","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1911.05082/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":"1911.05082","created_at":"2026-07-05T04:16:34.016899+00:00"},{"alias_kind":"arxiv_version","alias_value":"1911.05082v3","created_at":"2026-07-05T04:16:34.016899+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1911.05082","created_at":"2026-07-05T04:16:34.016899+00:00"},{"alias_kind":"pith_short_12","alias_value":"WAVYVJAT52MZ","created_at":"2026-07-05T04:16:34.016899+00:00"},{"alias_kind":"pith_short_16","alias_value":"WAVYVJAT52MZRCUH","created_at":"2026-07-05T04:16:34.016899+00:00"},{"alias_kind":"pith_short_8","alias_value":"WAVYVJAT","created_at":"2026-07-05T04:16:34.016899+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.03106","citing_title":"Holographic reconstruction for defect CFTs from $\\mathrm{AdS}_p \\times S^q$ spacetimes","ref_index":26,"is_internal_anchor":false},{"citing_arxiv_id":"2605.16482","citing_title":"When Symmetries Twist: Anomaly Inflow on Monodromy Defects","ref_index":26,"is_internal_anchor":false},{"citing_arxiv_id":"2605.16482","citing_title":"When Symmetries Twist: Anomaly Inflow on Monodromy Defects","ref_index":26,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WAVYVJAT52MZRCUHJRS5NQJ2XY","json":"https://pith.science/pith/WAVYVJAT52MZRCUHJRS5NQJ2XY.json","graph_json":"https://pith.science/api/pith-number/WAVYVJAT52MZRCUHJRS5NQJ2XY/graph.json","events_json":"https://pith.science/api/pith-number/WAVYVJAT52MZRCUHJRS5NQJ2XY/events.json","paper":"https://pith.science/paper/WAVYVJAT"},"agent_actions":{"view_html":"https://pith.science/pith/WAVYVJAT52MZRCUHJRS5NQJ2XY","download_json":"https://pith.science/pith/WAVYVJAT52MZRCUHJRS5NQJ2XY.json","view_paper":"https://pith.science/paper/WAVYVJAT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1911.05082&json=true","fetch_graph":"https://pith.science/api/pith-number/WAVYVJAT52MZRCUHJRS5NQJ2XY/graph.json","fetch_events":"https://pith.science/api/pith-number/WAVYVJAT52MZRCUHJRS5NQJ2XY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WAVYVJAT52MZRCUHJRS5NQJ2XY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WAVYVJAT52MZRCUHJRS5NQJ2XY/action/storage_attestation","attest_author":"https://pith.science/pith/WAVYVJAT52MZRCUHJRS5NQJ2XY/action/author_attestation","sign_citation":"https://pith.science/pith/WAVYVJAT52MZRCUHJRS5NQJ2XY/action/citation_signature","submit_replication":"https://pith.science/pith/WAVYVJAT52MZRCUHJRS5NQJ2XY/action/replication_record"}},"created_at":"2026-07-05T04:16:34.016899+00:00","updated_at":"2026-07-05T04:16:34.016899+00:00"}