{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:VW4VQY3QQCM2BNVRK5JCPOPYNS","short_pith_number":"pith:VW4VQY3Q","schema_version":"1.0","canonical_sha256":"adb95863708099a0b6b1575227b9f86cb851dbe3ef2a458cf60064d64ab7d8cc","source":{"kind":"arxiv","id":"0705.0752","version":1},"attestation_state":"computed","paper":{"title":"The E_{11} origin of all maximal supergravities","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Fabio Riccioni, Peter West","submitted_at":"2007-05-07T08:36:53Z","abstract_excerpt":"Starting from the eleven dimensional E_{11} non-linear realisation of M-theory we compute all possible forms, that is objects with totally antisymmetrised indices, that occur in four dimensions and above as well as all the 1-forms and 2-forms in three dimensions. In any dimension D, the D-1-forms lead to maximal supergravity theories with cosmological constants and they are in precise agreement with the patterns of gauging found in any dimension using supersymmetry. The D-forms correspond to the presence of space-filling branes which are crucial for the consistency of orientifold models and ha"},"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":"0705.0752","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2007-05-07T08:36:53Z","cross_cats_sorted":[],"title_canon_sha256":"d65a6c2291517ce4dfdaf9dd132c11b32e27625ee39ac20899a2f6f2fb03b2db","abstract_canon_sha256":"010e3b6995443985e5ea285435bcfc9320f020d244f93950b038ef4036ee2151"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:41:13.906261Z","signature_b64":"hXw12O2CY/f4eH1HX/+ukV6L+7PB1muwpq3cWfe2ORaDBuh2F3kW+8gwb0LvFSQC1wp16Ehj5DFyNhfant7NAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"adb95863708099a0b6b1575227b9f86cb851dbe3ef2a458cf60064d64ab7d8cc","last_reissued_at":"2026-07-04T15:41:13.905910Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:41:13.905910Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The E_{11} origin of all maximal supergravities","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Fabio Riccioni, Peter West","submitted_at":"2007-05-07T08:36:53Z","abstract_excerpt":"Starting from the eleven dimensional E_{11} non-linear realisation of M-theory we compute all possible forms, that is objects with totally antisymmetrised indices, that occur in four dimensions and above as well as all the 1-forms and 2-forms in three dimensions. In any dimension D, the D-1-forms lead to maximal supergravity theories with cosmological constants and they are in precise agreement with the patterns of gauging found in any dimension using supersymmetry. The D-forms correspond to the presence of space-filling branes which are crucial for the consistency of orientifold models and ha"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0705.0752","kind":"arxiv","version":1},"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/0705.0752/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":"0705.0752","created_at":"2026-07-04T15:41:13.905975+00:00"},{"alias_kind":"arxiv_version","alias_value":"0705.0752v1","created_at":"2026-07-04T15:41:13.905975+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0705.0752","created_at":"2026-07-04T15:41:13.905975+00:00"},{"alias_kind":"pith_short_12","alias_value":"VW4VQY3QQCM2","created_at":"2026-07-04T15:41:13.905975+00:00"},{"alias_kind":"pith_short_16","alias_value":"VW4VQY3QQCM2BNVR","created_at":"2026-07-04T15:41:13.905975+00:00"},{"alias_kind":"pith_short_8","alias_value":"VW4VQY3Q","created_at":"2026-07-04T15:41:13.905975+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2607.01999","citing_title":"Local symmetry and the dependence on extended spacetime","ref_index":23,"is_internal_anchor":true},{"citing_arxiv_id":"2603.11923","citing_title":"On the Sugawara Current Algebra Proposal for M-Theory","ref_index":12,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VW4VQY3QQCM2BNVRK5JCPOPYNS","json":"https://pith.science/pith/VW4VQY3QQCM2BNVRK5JCPOPYNS.json","graph_json":"https://pith.science/api/pith-number/VW4VQY3QQCM2BNVRK5JCPOPYNS/graph.json","events_json":"https://pith.science/api/pith-number/VW4VQY3QQCM2BNVRK5JCPOPYNS/events.json","paper":"https://pith.science/paper/VW4VQY3Q"},"agent_actions":{"view_html":"https://pith.science/pith/VW4VQY3QQCM2BNVRK5JCPOPYNS","download_json":"https://pith.science/pith/VW4VQY3QQCM2BNVRK5JCPOPYNS.json","view_paper":"https://pith.science/paper/VW4VQY3Q","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0705.0752&json=true","fetch_graph":"https://pith.science/api/pith-number/VW4VQY3QQCM2BNVRK5JCPOPYNS/graph.json","fetch_events":"https://pith.science/api/pith-number/VW4VQY3QQCM2BNVRK5JCPOPYNS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VW4VQY3QQCM2BNVRK5JCPOPYNS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VW4VQY3QQCM2BNVRK5JCPOPYNS/action/storage_attestation","attest_author":"https://pith.science/pith/VW4VQY3QQCM2BNVRK5JCPOPYNS/action/author_attestation","sign_citation":"https://pith.science/pith/VW4VQY3QQCM2BNVRK5JCPOPYNS/action/citation_signature","submit_replication":"https://pith.science/pith/VW4VQY3QQCM2BNVRK5JCPOPYNS/action/replication_record"}},"created_at":"2026-07-04T15:41:13.905975+00:00","updated_at":"2026-07-04T15:41:13.905975+00:00"}