{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:APOLPIBHYCGVCQYQ3GDMCVSW4K","short_pith_number":"pith:APOLPIBH","schema_version":"1.0","canonical_sha256":"03dcb7a027c08d514310d986c15656e2be21ee39c17bc11be450db6f0f65e558","source":{"kind":"arxiv","id":"2502.13613","version":2},"attestation_state":"computed","paper":{"title":"B-type anomaly coefficients for the D3-D7 domain wall","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Georgios Linardopoulos","submitted_at":"2025-02-19T10:48:50Z","abstract_excerpt":"We compute B-type Weyl anomaly coefficients for the two non-supersymmetric codimension-1 domain wall versions of N = 4 super Yang-Mills theory which are holographically dual to the D3-D7 probe-brane system. We compute the two-point function of the (improved) energy-momentum tensor in the presence of the domain wall, to leading order in perturbation theory. From it we determine the two-point function of the corresponding displacement operator and the b2 anomaly coefficient for both domain wall systems."},"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":"2502.13613","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2025-02-19T10:48:50Z","cross_cats_sorted":[],"title_canon_sha256":"010294a6eade021f2f5768c0993dbb49aad741ecdfec472af4b4c7c56ae26a88","abstract_canon_sha256":"5175fe62cc91628d81d3adf9ec948527c76c9af86cf10e072fc684c5566cbfa8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:30:41.600514Z","signature_b64":"LW2YFbqYXhAWpyLlYk8J/7aYhBe2OwC/4Lmn8C4ixJ4OIr81rDkrr6k+pxTAl+nOVc4LCrTWdSDTcuVqDeDRBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"03dcb7a027c08d514310d986c15656e2be21ee39c17bc11be450db6f0f65e558","last_reissued_at":"2026-07-05T11:30:41.599991Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:30:41.599991Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"B-type anomaly coefficients for the D3-D7 domain wall","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Georgios Linardopoulos","submitted_at":"2025-02-19T10:48:50Z","abstract_excerpt":"We compute B-type Weyl anomaly coefficients for the two non-supersymmetric codimension-1 domain wall versions of N = 4 super Yang-Mills theory which are holographically dual to the D3-D7 probe-brane system. We compute the two-point function of the (improved) energy-momentum tensor in the presence of the domain wall, to leading order in perturbation theory. From it we determine the two-point function of the corresponding displacement operator and the b2 anomaly coefficient for both domain wall systems."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.13613","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/2502.13613/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":"2502.13613","created_at":"2026-07-05T11:30:41.600052+00:00"},{"alias_kind":"arxiv_version","alias_value":"2502.13613v2","created_at":"2026-07-05T11:30:41.600052+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.13613","created_at":"2026-07-05T11:30:41.600052+00:00"},{"alias_kind":"pith_short_12","alias_value":"APOLPIBHYCGV","created_at":"2026-07-05T11:30:41.600052+00:00"},{"alias_kind":"pith_short_16","alias_value":"APOLPIBHYCGVCQYQ","created_at":"2026-07-05T11:30:41.600052+00:00"},{"alias_kind":"pith_short_8","alias_value":"APOLPIBH","created_at":"2026-07-05T11:30:41.600052+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.14505","citing_title":"Holography of a novel codimension-2 defect CFT","ref_index":32,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/APOLPIBHYCGVCQYQ3GDMCVSW4K","json":"https://pith.science/pith/APOLPIBHYCGVCQYQ3GDMCVSW4K.json","graph_json":"https://pith.science/api/pith-number/APOLPIBHYCGVCQYQ3GDMCVSW4K/graph.json","events_json":"https://pith.science/api/pith-number/APOLPIBHYCGVCQYQ3GDMCVSW4K/events.json","paper":"https://pith.science/paper/APOLPIBH"},"agent_actions":{"view_html":"https://pith.science/pith/APOLPIBHYCGVCQYQ3GDMCVSW4K","download_json":"https://pith.science/pith/APOLPIBHYCGVCQYQ3GDMCVSW4K.json","view_paper":"https://pith.science/paper/APOLPIBH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2502.13613&json=true","fetch_graph":"https://pith.science/api/pith-number/APOLPIBHYCGVCQYQ3GDMCVSW4K/graph.json","fetch_events":"https://pith.science/api/pith-number/APOLPIBHYCGVCQYQ3GDMCVSW4K/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/APOLPIBHYCGVCQYQ3GDMCVSW4K/action/timestamp_anchor","attest_storage":"https://pith.science/pith/APOLPIBHYCGVCQYQ3GDMCVSW4K/action/storage_attestation","attest_author":"https://pith.science/pith/APOLPIBHYCGVCQYQ3GDMCVSW4K/action/author_attestation","sign_citation":"https://pith.science/pith/APOLPIBHYCGVCQYQ3GDMCVSW4K/action/citation_signature","submit_replication":"https://pith.science/pith/APOLPIBHYCGVCQYQ3GDMCVSW4K/action/replication_record"}},"created_at":"2026-07-05T11:30:41.600052+00:00","updated_at":"2026-07-05T11:30:41.600052+00:00"}