{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:WSJUSZCPNTK23RTFPVAPPKHDMI","short_pith_number":"pith:WSJUSZCP","schema_version":"1.0","canonical_sha256":"b49349644f6cd5adc6657d40f7a8e36216ee407fc221c6953ac643133fabd8a0","source":{"kind":"arxiv","id":"1006.1646","version":1},"attestation_state":"computed","paper":{"title":"Mass-Deformed BLG Theory in Light-Cone Superspace","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dmitry V. Belyaev","submitted_at":"2010-06-08T19:57:05Z","abstract_excerpt":"Maximally supersymmetric mass deformation of the Bagger-Lambert-Gustavsson (BLG) theory corresponds to a {non-central} extension of the d=3 N=8 Poincare superalgebra (allowed in three dimensions). We obtain its light-cone superspace formulation which has a novel feature of the dynamical supersymmetry generators being {cubic} in the kinematical ones. The mass deformation picks a quaternionic direction, which breaks the SO(8) R-symmetry down to SO(4)xSO(4). The Hamiltonian of the theory is shown to be a quadratic form of the dynamical supersymmetry transformations, to all orders in the mass para"},"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":"1006.1646","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-06-08T19:57:05Z","cross_cats_sorted":[],"title_canon_sha256":"7d02b5e24a0280034a30f175378a735a20075ebe47590d76da4dc541cf208161","abstract_canon_sha256":"645c5536b2ce04c3e45f4cb4b7af7114b74fae920381852d86b5fb9768305e7c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:33:17.592763Z","signature_b64":"h5zx+wiZLM4IeDaIs+Wsn97y01VzZlcvXN9G2X9GcEr5wU4xYordqaq3KJN/eRcSrpUNxezsPjeECqX/KigHDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b49349644f6cd5adc6657d40f7a8e36216ee407fc221c6953ac643133fabd8a0","last_reissued_at":"2026-05-18T02:33:17.591766Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:33:17.591766Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Mass-Deformed BLG Theory in Light-Cone Superspace","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dmitry V. Belyaev","submitted_at":"2010-06-08T19:57:05Z","abstract_excerpt":"Maximally supersymmetric mass deformation of the Bagger-Lambert-Gustavsson (BLG) theory corresponds to a {non-central} extension of the d=3 N=8 Poincare superalgebra (allowed in three dimensions). We obtain its light-cone superspace formulation which has a novel feature of the dynamical supersymmetry generators being {cubic} in the kinematical ones. The mass deformation picks a quaternionic direction, which breaks the SO(8) R-symmetry down to SO(4)xSO(4). The Hamiltonian of the theory is shown to be a quadratic form of the dynamical supersymmetry transformations, to all orders in the mass para"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1006.1646","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":""},"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":"1006.1646","created_at":"2026-05-18T02:33:17.591870+00:00"},{"alias_kind":"arxiv_version","alias_value":"1006.1646v1","created_at":"2026-05-18T02:33:17.591870+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1006.1646","created_at":"2026-05-18T02:33:17.591870+00:00"},{"alias_kind":"pith_short_12","alias_value":"WSJUSZCPNTK2","created_at":"2026-05-18T12:26:17.028572+00:00"},{"alias_kind":"pith_short_16","alias_value":"WSJUSZCPNTK23RTF","created_at":"2026-05-18T12:26:17.028572+00:00"},{"alias_kind":"pith_short_8","alias_value":"WSJUSZCP","created_at":"2026-05-18T12:26:17.028572+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WSJUSZCPNTK23RTFPVAPPKHDMI","json":"https://pith.science/pith/WSJUSZCPNTK23RTFPVAPPKHDMI.json","graph_json":"https://pith.science/api/pith-number/WSJUSZCPNTK23RTFPVAPPKHDMI/graph.json","events_json":"https://pith.science/api/pith-number/WSJUSZCPNTK23RTFPVAPPKHDMI/events.json","paper":"https://pith.science/paper/WSJUSZCP"},"agent_actions":{"view_html":"https://pith.science/pith/WSJUSZCPNTK23RTFPVAPPKHDMI","download_json":"https://pith.science/pith/WSJUSZCPNTK23RTFPVAPPKHDMI.json","view_paper":"https://pith.science/paper/WSJUSZCP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1006.1646&json=true","fetch_graph":"https://pith.science/api/pith-number/WSJUSZCPNTK23RTFPVAPPKHDMI/graph.json","fetch_events":"https://pith.science/api/pith-number/WSJUSZCPNTK23RTFPVAPPKHDMI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WSJUSZCPNTK23RTFPVAPPKHDMI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WSJUSZCPNTK23RTFPVAPPKHDMI/action/storage_attestation","attest_author":"https://pith.science/pith/WSJUSZCPNTK23RTFPVAPPKHDMI/action/author_attestation","sign_citation":"https://pith.science/pith/WSJUSZCPNTK23RTFPVAPPKHDMI/action/citation_signature","submit_replication":"https://pith.science/pith/WSJUSZCPNTK23RTFPVAPPKHDMI/action/replication_record"}},"created_at":"2026-05-18T02:33:17.591870+00:00","updated_at":"2026-05-18T02:33:17.591870+00:00"}