{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:2LRPAX67CPFT7SKFF544BBOJLD","short_pith_number":"pith:2LRPAX67","schema_version":"1.0","canonical_sha256":"d2e2f05fdf13cb3fc9452f79c085c958f1441ead45659c86e34a990a3aee1b79","source":{"kind":"arxiv","id":"1908.03278","version":2},"attestation_state":"computed","paper":{"title":"Rank $Q$ E-string on a torus with flux","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Gabi Zafrir, Matteo Sacchi, Sara Pasquetti, Shlomo S. Razamat","submitted_at":"2019-08-08T22:16:25Z","abstract_excerpt":"We discuss compactifications of rank $Q$ E-string theory on a torus with fluxes for abelian subgroups of the $E_8$ global symmetry of the $6d$ SCFT. We argue that the theories corresponding to such tori are built from a simple model we denote as $E[USp(2Q)]$. This model has a variety of non trivial properties. In particular the global symmetry is $USp(2Q)\\times USp(2Q)\\times U(1)^2$ with one of the two $USp(2Q)$ symmetries emerging in the IR as an enhancement of an $SU(2)^Q$ symmetry of the UV Lagrangian. The $E[USp(2Q)]$ model after dimensional reduction to $3d$ and a subsequent Coulomb branc"},"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":"1908.03278","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-08-08T22:16:25Z","cross_cats_sorted":[],"title_canon_sha256":"8eec83be9f6b46d7fb0c419f5779839554bd3a4bebd4f02bf14d816c99970d95","abstract_canon_sha256":"a5bf7f88b7fd023a6221e7a36ec6aa0e5328e51e5aae37e4efda128f1becec4f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:36:59.302045Z","signature_b64":"B2B3VjuoPighXBZrs5vAEdL+ZKAuXuFO9SThYiNIZNv2Kf66jDV3RKiAgJ9S82m9DBODfZdsOXvz032urvnHBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d2e2f05fdf13cb3fc9452f79c085c958f1441ead45659c86e34a990a3aee1b79","last_reissued_at":"2026-07-05T00:36:59.301438Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:36:59.301438Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Rank $Q$ E-string on a torus with flux","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Gabi Zafrir, Matteo Sacchi, Sara Pasquetti, Shlomo S. Razamat","submitted_at":"2019-08-08T22:16:25Z","abstract_excerpt":"We discuss compactifications of rank $Q$ E-string theory on a torus with fluxes for abelian subgroups of the $E_8$ global symmetry of the $6d$ SCFT. We argue that the theories corresponding to such tori are built from a simple model we denote as $E[USp(2Q)]$. This model has a variety of non trivial properties. In particular the global symmetry is $USp(2Q)\\times USp(2Q)\\times U(1)^2$ with one of the two $USp(2Q)$ symmetries emerging in the IR as an enhancement of an $SU(2)^Q$ symmetry of the UV Lagrangian. The $E[USp(2Q)]$ model after dimensional reduction to $3d$ and a subsequent Coulomb branc"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1908.03278","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/1908.03278/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":"1908.03278","created_at":"2026-07-05T00:36:59.301511+00:00"},{"alias_kind":"arxiv_version","alias_value":"1908.03278v2","created_at":"2026-07-05T00:36:59.301511+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1908.03278","created_at":"2026-07-05T00:36:59.301511+00:00"},{"alias_kind":"pith_short_12","alias_value":"2LRPAX67CPFT","created_at":"2026-07-05T00:36:59.301511+00:00"},{"alias_kind":"pith_short_16","alias_value":"2LRPAX67CPFT7SKF","created_at":"2026-07-05T00:36:59.301511+00:00"},{"alias_kind":"pith_short_8","alias_value":"2LRPAX67","created_at":"2026-07-05T00:36:59.301511+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.19885","citing_title":"On non-relativistic integrable models and 4d SCFTs","ref_index":118,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2LRPAX67CPFT7SKFF544BBOJLD","json":"https://pith.science/pith/2LRPAX67CPFT7SKFF544BBOJLD.json","graph_json":"https://pith.science/api/pith-number/2LRPAX67CPFT7SKFF544BBOJLD/graph.json","events_json":"https://pith.science/api/pith-number/2LRPAX67CPFT7SKFF544BBOJLD/events.json","paper":"https://pith.science/paper/2LRPAX67"},"agent_actions":{"view_html":"https://pith.science/pith/2LRPAX67CPFT7SKFF544BBOJLD","download_json":"https://pith.science/pith/2LRPAX67CPFT7SKFF544BBOJLD.json","view_paper":"https://pith.science/paper/2LRPAX67","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1908.03278&json=true","fetch_graph":"https://pith.science/api/pith-number/2LRPAX67CPFT7SKFF544BBOJLD/graph.json","fetch_events":"https://pith.science/api/pith-number/2LRPAX67CPFT7SKFF544BBOJLD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2LRPAX67CPFT7SKFF544BBOJLD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2LRPAX67CPFT7SKFF544BBOJLD/action/storage_attestation","attest_author":"https://pith.science/pith/2LRPAX67CPFT7SKFF544BBOJLD/action/author_attestation","sign_citation":"https://pith.science/pith/2LRPAX67CPFT7SKFF544BBOJLD/action/citation_signature","submit_replication":"https://pith.science/pith/2LRPAX67CPFT7SKFF544BBOJLD/action/replication_record"}},"created_at":"2026-07-05T00:36:59.301511+00:00","updated_at":"2026-07-05T00:36:59.301511+00:00"}