{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:JGYULNCLO4KMEQJPFZSKMBES2O","short_pith_number":"pith:JGYULNCL","schema_version":"1.0","canonical_sha256":"49b145b44b7714c2412f2e64a60492d3beb21c683af7eee2f7a735e62ac3e4c4","source":{"kind":"arxiv","id":"hep-th/0502245","version":1},"attestation_state":"computed","paper":{"title":"Two-dimensional N=8 supersymmetric mechanics in superspace","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Shcherbakov, S. Bellucci, S. Krivonos","submitted_at":"2005-02-28T15:47:43Z","abstract_excerpt":"We construct a two-dimensional N=8 supersymmetric quantum mechanics which inherits the most interesting properties of N=2, $d=4$ supersymmetric Yang-Mills theory. After dimensional reduction to one dimension in terms of field-strength, we show that only complex scalar fields from the $N=2, d=4$ vector multiplet become physical bosons in $d=1$. The rest of the bosonic components are reduced to auxiliary fields, thus giving rise to the {\\bf (2, 8, 6)} supermultiplet in $d=1$. We construct the most general superfields action for this supermultiplet and demonstrate that it possesses duality symmet"},"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":"hep-th/0502245","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2005-02-28T15:47:43Z","cross_cats_sorted":[],"title_canon_sha256":"ef613410d037439c69e7386f306cf482d5b417f027e0cb68f97dc300f718f68a","abstract_canon_sha256":"68067801d757a719d4b8b96d7fd6969e5fcc86f085e9b1b8ca250316757870de"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:56:05.802745Z","signature_b64":"0JqUsbSg6GnLuK5d3Zr7dT9dygU90vLz1Nw/+3XFg2nOuG9GhLbr7q7OX7mNdZb8LGT7aJ3w3FpV5bnMAIdqBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"49b145b44b7714c2412f2e64a60492d3beb21c683af7eee2f7a735e62ac3e4c4","last_reissued_at":"2026-07-04T16:56:05.802390Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:56:05.802390Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Two-dimensional N=8 supersymmetric mechanics in superspace","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Shcherbakov, S. Bellucci, S. Krivonos","submitted_at":"2005-02-28T15:47:43Z","abstract_excerpt":"We construct a two-dimensional N=8 supersymmetric quantum mechanics which inherits the most interesting properties of N=2, $d=4$ supersymmetric Yang-Mills theory. After dimensional reduction to one dimension in terms of field-strength, we show that only complex scalar fields from the $N=2, d=4$ vector multiplet become physical bosons in $d=1$. The rest of the bosonic components are reduced to auxiliary fields, thus giving rise to the {\\bf (2, 8, 6)} supermultiplet in $d=1$. We construct the most general superfields action for this supermultiplet and demonstrate that it possesses duality symmet"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0502245","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/hep-th/0502245/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":"hep-th/0502245","created_at":"2026-07-04T16:56:05.802453+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0502245v1","created_at":"2026-07-04T16:56:05.802453+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0502245","created_at":"2026-07-04T16:56:05.802453+00:00"},{"alias_kind":"pith_short_12","alias_value":"JGYULNCLO4KM","created_at":"2026-07-04T16:56:05.802453+00:00"},{"alias_kind":"pith_short_16","alias_value":"JGYULNCLO4KMEQJP","created_at":"2026-07-04T16:56:05.802453+00:00"},{"alias_kind":"pith_short_8","alias_value":"JGYULNCL","created_at":"2026-07-04T16:56:05.802453+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1908.06490","citing_title":"Geometry and integrability in $\\mathcal{N}=8$ supersymmetric mechanics","ref_index":19,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JGYULNCLO4KMEQJPFZSKMBES2O","json":"https://pith.science/pith/JGYULNCLO4KMEQJPFZSKMBES2O.json","graph_json":"https://pith.science/api/pith-number/JGYULNCLO4KMEQJPFZSKMBES2O/graph.json","events_json":"https://pith.science/api/pith-number/JGYULNCLO4KMEQJPFZSKMBES2O/events.json","paper":"https://pith.science/paper/JGYULNCL"},"agent_actions":{"view_html":"https://pith.science/pith/JGYULNCLO4KMEQJPFZSKMBES2O","download_json":"https://pith.science/pith/JGYULNCLO4KMEQJPFZSKMBES2O.json","view_paper":"https://pith.science/paper/JGYULNCL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0502245&json=true","fetch_graph":"https://pith.science/api/pith-number/JGYULNCLO4KMEQJPFZSKMBES2O/graph.json","fetch_events":"https://pith.science/api/pith-number/JGYULNCLO4KMEQJPFZSKMBES2O/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JGYULNCLO4KMEQJPFZSKMBES2O/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JGYULNCLO4KMEQJPFZSKMBES2O/action/storage_attestation","attest_author":"https://pith.science/pith/JGYULNCLO4KMEQJPFZSKMBES2O/action/author_attestation","sign_citation":"https://pith.science/pith/JGYULNCLO4KMEQJPFZSKMBES2O/action/citation_signature","submit_replication":"https://pith.science/pith/JGYULNCLO4KMEQJPFZSKMBES2O/action/replication_record"}},"created_at":"2026-07-04T16:56:05.802453+00:00","updated_at":"2026-07-04T16:56:05.802453+00:00"}