{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:FQTFTWHEATM3XVUJKOAPB735AW","short_pith_number":"pith:FQTFTWHE","schema_version":"1.0","canonical_sha256":"2c2659d8e404d9bbd6895380f0ff7d058a29edd639ca769eb771b5529c3983c4","source":{"kind":"arxiv","id":"1811.11231","version":3},"attestation_state":"computed","paper":{"title":"M2-branes on a constant flux background","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Restuccia, C. Las Heras, J.M. Pena, M.P. Garcia del Moral, P. Leon","submitted_at":"2018-11-27T20:06:00Z","abstract_excerpt":"We describe a compactified Supermembrane, or M2-brane, with 2-form fluxes generated by constant three-forms that are turned on a 2-torus of the target space $M_9\\times T^2$. We compare this theory with the one describing a $11D$ M2-brane formulated on $M_9\\times T^2$ target space subject to an irreducible wrapping condition. We show that the flux generated by the bosonic 3-form under consideration is in a one to one correspondence to the irreducible wrapping condition. After a canonical transformation both Hamiltonians are exactly the same up to a constant shift in one particular case. Consequ"},"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":"1811.11231","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-11-27T20:06:00Z","cross_cats_sorted":[],"title_canon_sha256":"22d89c82f4b22a69f45663cffd396dc8094273f2d31eed083dd4c82f62b87626","abstract_canon_sha256":"fb2a90c02900abe409cd8bb9d0fbc3a599d7ef180fed8376ce38436e3947db81"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:03:30.825967Z","signature_b64":"rso40w+TK+fd3T1dhMS7S19458ccLJAvnGFvX5HhxuxWCPJTCVnxQV4LfAxiLfMxwjj/x/Eoq0AFTYUs8pd/Dw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2c2659d8e404d9bbd6895380f0ff7d058a29edd639ca769eb771b5529c3983c4","last_reissued_at":"2026-07-05T00:03:30.825557Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:03:30.825557Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"M2-branes on a constant flux background","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Restuccia, C. Las Heras, J.M. Pena, M.P. Garcia del Moral, P. Leon","submitted_at":"2018-11-27T20:06:00Z","abstract_excerpt":"We describe a compactified Supermembrane, or M2-brane, with 2-form fluxes generated by constant three-forms that are turned on a 2-torus of the target space $M_9\\times T^2$. We compare this theory with the one describing a $11D$ M2-brane formulated on $M_9\\times T^2$ target space subject to an irreducible wrapping condition. We show that the flux generated by the bosonic 3-form under consideration is in a one to one correspondence to the irreducible wrapping condition. After a canonical transformation both Hamiltonians are exactly the same up to a constant shift in one particular case. Consequ"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.11231","kind":"arxiv","version":3},"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/1811.11231/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":"1811.11231","created_at":"2026-07-05T00:03:30.825619+00:00"},{"alias_kind":"arxiv_version","alias_value":"1811.11231v3","created_at":"2026-07-05T00:03:30.825619+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.11231","created_at":"2026-07-05T00:03:30.825619+00:00"},{"alias_kind":"pith_short_12","alias_value":"FQTFTWHEATM3","created_at":"2026-07-05T00:03:30.825619+00:00"},{"alias_kind":"pith_short_16","alias_value":"FQTFTWHEATM3XVUJ","created_at":"2026-07-05T00:03:30.825619+00:00"},{"alias_kind":"pith_short_8","alias_value":"FQTFTWHE","created_at":"2026-07-05T00:03:30.825619+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.07924","citing_title":"2-Group global symmetry in the compactified M2-brane","ref_index":19,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FQTFTWHEATM3XVUJKOAPB735AW","json":"https://pith.science/pith/FQTFTWHEATM3XVUJKOAPB735AW.json","graph_json":"https://pith.science/api/pith-number/FQTFTWHEATM3XVUJKOAPB735AW/graph.json","events_json":"https://pith.science/api/pith-number/FQTFTWHEATM3XVUJKOAPB735AW/events.json","paper":"https://pith.science/paper/FQTFTWHE"},"agent_actions":{"view_html":"https://pith.science/pith/FQTFTWHEATM3XVUJKOAPB735AW","download_json":"https://pith.science/pith/FQTFTWHEATM3XVUJKOAPB735AW.json","view_paper":"https://pith.science/paper/FQTFTWHE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1811.11231&json=true","fetch_graph":"https://pith.science/api/pith-number/FQTFTWHEATM3XVUJKOAPB735AW/graph.json","fetch_events":"https://pith.science/api/pith-number/FQTFTWHEATM3XVUJKOAPB735AW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FQTFTWHEATM3XVUJKOAPB735AW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FQTFTWHEATM3XVUJKOAPB735AW/action/storage_attestation","attest_author":"https://pith.science/pith/FQTFTWHEATM3XVUJKOAPB735AW/action/author_attestation","sign_citation":"https://pith.science/pith/FQTFTWHEATM3XVUJKOAPB735AW/action/citation_signature","submit_replication":"https://pith.science/pith/FQTFTWHEATM3XVUJKOAPB735AW/action/replication_record"}},"created_at":"2026-07-05T00:03:30.825619+00:00","updated_at":"2026-07-05T00:03:30.825619+00:00"}