{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:WUPJVVBD44HDZIWYTE6G73OVF7","short_pith_number":"pith:WUPJVVBD","schema_version":"1.0","canonical_sha256":"b51e9ad423e70e3ca2d8993c6fedd52fda64cf7c6341c007c1349baefe5678e2","source":{"kind":"arxiv","id":"1906.10709","version":4},"attestation_state":"computed","paper":{"title":"Exceptional Super Yang-Mills in $D=27+3$ and Worldvolume M-Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alessio Marrani, David Chester, Michael Rios","submitted_at":"2019-06-25T18:01:01Z","abstract_excerpt":"Bars and Sezgin have proposed a super Yang-Mills theory in $D=s+t=11+3$ space-time dimensions with an electric 3-brane that generalizes the 2-brane of M-theory. More recently, the authors found an infinite family of exceptional super Yang-Mills theories in $D=(8n+3)+3$ via the so-called Magic Star algebras. A particularly interesting case occurs in signature $D=27+3$, where the superalgebra is centrally extended by an electric 11-brane and its 15-brane magnetic dual. The worldvolume symmetry of the 11-brane has signature $D=11+3$ and can reproduce super Yang-Mills theory in $D=11+3$. Upon redu"},"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":"1906.10709","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-06-25T18:01:01Z","cross_cats_sorted":[],"title_canon_sha256":"7bdf17cb9d23ce842b38968cf40728850b75cec89734174ea691b74404db80ec","abstract_canon_sha256":"8c20344b456e6b240c3f328033d75da5d9a862663009c44ed7c23db071131dd7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:33:33.489818Z","signature_b64":"6lb5ElF6h2WyCcfa92agXeTQEhlAUZdObOppxWbx85zWBsFMDPulqgdWojnniM9CY38rX0Z9p/CbAHzcyrCTDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b51e9ad423e70e3ca2d8993c6fedd52fda64cf7c6341c007c1349baefe5678e2","last_reissued_at":"2026-07-05T01:33:33.489345Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:33:33.489345Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Exceptional Super Yang-Mills in $D=27+3$ and Worldvolume M-Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alessio Marrani, David Chester, Michael Rios","submitted_at":"2019-06-25T18:01:01Z","abstract_excerpt":"Bars and Sezgin have proposed a super Yang-Mills theory in $D=s+t=11+3$ space-time dimensions with an electric 3-brane that generalizes the 2-brane of M-theory. More recently, the authors found an infinite family of exceptional super Yang-Mills theories in $D=(8n+3)+3$ via the so-called Magic Star algebras. A particularly interesting case occurs in signature $D=27+3$, where the superalgebra is centrally extended by an electric 11-brane and its 15-brane magnetic dual. The worldvolume symmetry of the 11-brane has signature $D=11+3$ and can reproduce super Yang-Mills theory in $D=11+3$. Upon redu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1906.10709","kind":"arxiv","version":4},"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/1906.10709/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":"1906.10709","created_at":"2026-07-05T01:33:33.489402+00:00"},{"alias_kind":"arxiv_version","alias_value":"1906.10709v4","created_at":"2026-07-05T01:33:33.489402+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1906.10709","created_at":"2026-07-05T01:33:33.489402+00:00"},{"alias_kind":"pith_short_12","alias_value":"WUPJVVBD44HD","created_at":"2026-07-05T01:33:33.489402+00:00"},{"alias_kind":"pith_short_16","alias_value":"WUPJVVBD44HDZIWY","created_at":"2026-07-05T01:33:33.489402+00:00"},{"alias_kind":"pith_short_8","alias_value":"WUPJVVBD","created_at":"2026-07-05T01:33:33.489402+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.20191","citing_title":"Flipped $SU(5)$ GUT with conformal gravity from a single supermultiplet","ref_index":63,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WUPJVVBD44HDZIWYTE6G73OVF7","json":"https://pith.science/pith/WUPJVVBD44HDZIWYTE6G73OVF7.json","graph_json":"https://pith.science/api/pith-number/WUPJVVBD44HDZIWYTE6G73OVF7/graph.json","events_json":"https://pith.science/api/pith-number/WUPJVVBD44HDZIWYTE6G73OVF7/events.json","paper":"https://pith.science/paper/WUPJVVBD"},"agent_actions":{"view_html":"https://pith.science/pith/WUPJVVBD44HDZIWYTE6G73OVF7","download_json":"https://pith.science/pith/WUPJVVBD44HDZIWYTE6G73OVF7.json","view_paper":"https://pith.science/paper/WUPJVVBD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1906.10709&json=true","fetch_graph":"https://pith.science/api/pith-number/WUPJVVBD44HDZIWYTE6G73OVF7/graph.json","fetch_events":"https://pith.science/api/pith-number/WUPJVVBD44HDZIWYTE6G73OVF7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WUPJVVBD44HDZIWYTE6G73OVF7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WUPJVVBD44HDZIWYTE6G73OVF7/action/storage_attestation","attest_author":"https://pith.science/pith/WUPJVVBD44HDZIWYTE6G73OVF7/action/author_attestation","sign_citation":"https://pith.science/pith/WUPJVVBD44HDZIWYTE6G73OVF7/action/citation_signature","submit_replication":"https://pith.science/pith/WUPJVVBD44HDZIWYTE6G73OVF7/action/replication_record"}},"created_at":"2026-07-05T01:33:33.489402+00:00","updated_at":"2026-07-05T01:33:33.489402+00:00"}