{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:GWMFWCSKD46YMKIWYXQ4Y67OOH","short_pith_number":"pith:GWMFWCSK","schema_version":"1.0","canonical_sha256":"35985b0a4a1f3d862916c5e1cc7bee71dc0d39ba1a66a83719af0a06561d9774","source":{"kind":"arxiv","id":"hep-th/0106165","version":2},"attestation_state":"computed","paper":{"title":"Anomaly of (2,0) Theories","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Piljin Yi","submitted_at":"2001-06-19T04:25:00Z","abstract_excerpt":"We compute gravitational and axial anomaly for D-type (2,0) theories realized on N pairs of coincident M5-branes at R^5/Z_2 orbifold fixed point. We first summarize work by Harvey, Minasian, and Moore on A-type (2,0) theories, and then extend it to include the effect of orbifold fixed point. The net anomaly inflow follows when we further take into account the consistency of T^5/Z_2 M-theory orbifold. We deduce that the world-volume anomaly is given by N{\\cal J}_8 + N(2N-1)(2N-2) p_2/24 where {\\cal J}_8 is the anomaly polynomial of a free tensor multiplet and p_2 is the second Pontryagin class "},"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/0106165","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2001-06-19T04:25:00Z","cross_cats_sorted":[],"title_canon_sha256":"d8741ff695e50da01bf70f149738bde3ec3820ca97aa503e2be54c219958985d","abstract_canon_sha256":"0a3759c8326fbd283392048156ff62a075deb6d6b6e909313102fe7937424952"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:27:54.895525Z","signature_b64":"bi/ej3xb4TvO9RJnL2uCBOeRxzEUKr0U3/Gmg3PJ+cA5Z3Ni/E3j4zyHsrz0/65/mT/yHAzpOMoqgD4D7+RkBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"35985b0a4a1f3d862916c5e1cc7bee71dc0d39ba1a66a83719af0a06561d9774","last_reissued_at":"2026-07-04T16:27:54.895156Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:27:54.895156Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Anomaly of (2,0) Theories","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Piljin Yi","submitted_at":"2001-06-19T04:25:00Z","abstract_excerpt":"We compute gravitational and axial anomaly for D-type (2,0) theories realized on N pairs of coincident M5-branes at R^5/Z_2 orbifold fixed point. We first summarize work by Harvey, Minasian, and Moore on A-type (2,0) theories, and then extend it to include the effect of orbifold fixed point. The net anomaly inflow follows when we further take into account the consistency of T^5/Z_2 M-theory orbifold. We deduce that the world-volume anomaly is given by N{\\cal J}_8 + N(2N-1)(2N-2) p_2/24 where {\\cal J}_8 is the anomaly polynomial of a free tensor multiplet and p_2 is the second Pontryagin class "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0106165","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/hep-th/0106165/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/0106165","created_at":"2026-07-04T16:27:54.895221+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0106165v2","created_at":"2026-07-04T16:27:54.895221+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0106165","created_at":"2026-07-04T16:27:54.895221+00:00"},{"alias_kind":"pith_short_12","alias_value":"GWMFWCSKD46Y","created_at":"2026-07-04T16:27:54.895221+00:00"},{"alias_kind":"pith_short_16","alias_value":"GWMFWCSKD46YMKIW","created_at":"2026-07-04T16:27:54.895221+00:00"},{"alias_kind":"pith_short_8","alias_value":"GWMFWCSK","created_at":"2026-07-04T16:27:54.895221+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.05884","citing_title":"A Crash Course in Supersymmetric Field Theory Across Dimensions","ref_index":65,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GWMFWCSKD46YMKIWYXQ4Y67OOH","json":"https://pith.science/pith/GWMFWCSKD46YMKIWYXQ4Y67OOH.json","graph_json":"https://pith.science/api/pith-number/GWMFWCSKD46YMKIWYXQ4Y67OOH/graph.json","events_json":"https://pith.science/api/pith-number/GWMFWCSKD46YMKIWYXQ4Y67OOH/events.json","paper":"https://pith.science/paper/GWMFWCSK"},"agent_actions":{"view_html":"https://pith.science/pith/GWMFWCSKD46YMKIWYXQ4Y67OOH","download_json":"https://pith.science/pith/GWMFWCSKD46YMKIWYXQ4Y67OOH.json","view_paper":"https://pith.science/paper/GWMFWCSK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0106165&json=true","fetch_graph":"https://pith.science/api/pith-number/GWMFWCSKD46YMKIWYXQ4Y67OOH/graph.json","fetch_events":"https://pith.science/api/pith-number/GWMFWCSKD46YMKIWYXQ4Y67OOH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GWMFWCSKD46YMKIWYXQ4Y67OOH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GWMFWCSKD46YMKIWYXQ4Y67OOH/action/storage_attestation","attest_author":"https://pith.science/pith/GWMFWCSKD46YMKIWYXQ4Y67OOH/action/author_attestation","sign_citation":"https://pith.science/pith/GWMFWCSKD46YMKIWYXQ4Y67OOH/action/citation_signature","submit_replication":"https://pith.science/pith/GWMFWCSKD46YMKIWYXQ4Y67OOH/action/replication_record"}},"created_at":"2026-07-04T16:27:54.895221+00:00","updated_at":"2026-07-04T16:27:54.895221+00:00"}