{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:5FKDZERVKB26DQZFKQCCG2VPJ4","short_pith_number":"pith:5FKDZERV","schema_version":"1.0","canonical_sha256":"e9543c92355075e1c3255404236aaf4f2b896d89700a893eab2434a346de4841","source":{"kind":"arxiv","id":"2510.00123","version":2},"attestation_state":"computed","paper":{"title":"Entanglement C-functions of defects and interfaces in $\\mathcal{N}=4$ supersymmetric Yang-Mills theory","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Helime Ruotsalainen, Jani Kastikainen, Jos\\'e Manuel Pen\\'in, Niko Jokela, Ronnie Rodgers","submitted_at":"2025-09-30T18:04:07Z","abstract_excerpt":"We consider planar codimension-one defects and interfaces in $\\mathcal{N}=4$ supersymmetric Yang-Mills (SYM) theory, realized by the D3/D5-brane intersection. Working in the probe limit, where the number of D5-branes is small compared to the number of D3-branes, we obtain analytic results for the holographic entanglement entropy of a ball-shaped region centered on the defect. A defect renormalization group flow is triggered by giving the defect hypermultiplets a mass, which corresponds to separating the D3- and D5-branes. Along this flow the entanglement C-function decreases monotonically. 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":"2510.00123","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2025-09-30T18:04:07Z","cross_cats_sorted":[],"title_canon_sha256":"7816b551335dfe1181c60919b67374c0e25fafaabacbc624778e21613c72aec1","abstract_canon_sha256":"eaa1a8fa1f267e4ed647293fca8815987b7946a83aec12734d8d8fc82196939b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-01T01:03:45.662546Z","signature_b64":"+qNLuO3W/TmEJQ3fIX5qYzqoEJffle/2MS+8H/D6/apmOVCWrnA0zvRiW2vca4PPiFTE8Q6EEQ/40wGt+U3NBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e9543c92355075e1c3255404236aaf4f2b896d89700a893eab2434a346de4841","last_reissued_at":"2026-06-01T01:03:45.661281Z","signature_status":"signed_v1","first_computed_at":"2026-06-01T01:03:45.661281Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Entanglement C-functions of defects and interfaces in $\\mathcal{N}=4$ supersymmetric Yang-Mills theory","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Helime Ruotsalainen, Jani Kastikainen, Jos\\'e Manuel Pen\\'in, Niko Jokela, Ronnie Rodgers","submitted_at":"2025-09-30T18:04:07Z","abstract_excerpt":"We consider planar codimension-one defects and interfaces in $\\mathcal{N}=4$ supersymmetric Yang-Mills (SYM) theory, realized by the D3/D5-brane intersection. Working in the probe limit, where the number of D5-branes is small compared to the number of D3-branes, we obtain analytic results for the holographic entanglement entropy of a ball-shaped region centered on the defect. A defect renormalization group flow is triggered by giving the defect hypermultiplets a mass, which corresponds to separating the D3- and D5-branes. Along this flow the entanglement C-function decreases monotonically. We "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2510.00123","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2510.00123/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":"2510.00123","created_at":"2026-06-01T01:03:45.661471+00:00"},{"alias_kind":"arxiv_version","alias_value":"2510.00123v2","created_at":"2026-06-01T01:03:45.661471+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2510.00123","created_at":"2026-06-01T01:03:45.661471+00:00"},{"alias_kind":"pith_short_12","alias_value":"5FKDZERVKB26","created_at":"2026-06-01T01:03:45.661471+00:00"},{"alias_kind":"pith_short_16","alias_value":"5FKDZERVKB26DQZF","created_at":"2026-06-01T01:03:45.661471+00:00"},{"alias_kind":"pith_short_8","alias_value":"5FKDZERV","created_at":"2026-06-01T01:03:45.661471+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5FKDZERVKB26DQZFKQCCG2VPJ4","json":"https://pith.science/pith/5FKDZERVKB26DQZFKQCCG2VPJ4.json","graph_json":"https://pith.science/api/pith-number/5FKDZERVKB26DQZFKQCCG2VPJ4/graph.json","events_json":"https://pith.science/api/pith-number/5FKDZERVKB26DQZFKQCCG2VPJ4/events.json","paper":"https://pith.science/paper/5FKDZERV"},"agent_actions":{"view_html":"https://pith.science/pith/5FKDZERVKB26DQZFKQCCG2VPJ4","download_json":"https://pith.science/pith/5FKDZERVKB26DQZFKQCCG2VPJ4.json","view_paper":"https://pith.science/paper/5FKDZERV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2510.00123&json=true","fetch_graph":"https://pith.science/api/pith-number/5FKDZERVKB26DQZFKQCCG2VPJ4/graph.json","fetch_events":"https://pith.science/api/pith-number/5FKDZERVKB26DQZFKQCCG2VPJ4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5FKDZERVKB26DQZFKQCCG2VPJ4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5FKDZERVKB26DQZFKQCCG2VPJ4/action/storage_attestation","attest_author":"https://pith.science/pith/5FKDZERVKB26DQZFKQCCG2VPJ4/action/author_attestation","sign_citation":"https://pith.science/pith/5FKDZERVKB26DQZFKQCCG2VPJ4/action/citation_signature","submit_replication":"https://pith.science/pith/5FKDZERVKB26DQZFKQCCG2VPJ4/action/replication_record"}},"created_at":"2026-06-01T01:03:45.661471+00:00","updated_at":"2026-06-01T01:03:45.661471+00:00"}