{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:CV4JKNQ7RIWS53BJEYEO2IBX36","short_pith_number":"pith:CV4JKNQ7","schema_version":"1.0","canonical_sha256":"157895361f8a2d2eec292608ed2037dfbf03d2c85e3d0f0f6eb3aafc03a08600","source":{"kind":"arxiv","id":"1905.11673","version":2},"attestation_state":"computed","paper":{"title":"Extended supersymmetry with central charges in Dirac action with curved extra dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","quant-ph"],"primary_cat":"hep-th","authors_text":"Inori Ueba","submitted_at":"2019-05-28T08:28:50Z","abstract_excerpt":"We discuss a new realization of $\\mathcal{N}$-extended quantum-mechanical supersymmetry (QM SUSY) with central charges hidden in the four-dimensional (4D) mass spectrum of higher dimensional Dirac action with curved extra dimensions. We show that this $\\mathcal{N}$-extended QM SUSY results from symmetries in extra dimensions, and the supermultiplets in this supersymmetry algebra correspond to the Bogomol'nyi--Prasad--Sommerfield states. Furthermore, we examine the model of the $S^2$ extra dimension with a magnetic monopole background and confirm that the $\\mathcal{N}$-extended QM SUSY explains"},"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":"1905.11673","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-05-28T08:28:50Z","cross_cats_sorted":["hep-ph","quant-ph"],"title_canon_sha256":"0ac7392b633190809c918dadc115a09d17ff3e6cdb2840bbd848402f9df7cec7","abstract_canon_sha256":"10a0b36ed1ed0cb77cec8951eb66f031b239d50b154b8badd7b0998e5d2c3c3f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:17:04.536991Z","signature_b64":"VXoZNW/6kKewvsMUYSw+FgZ3mEVAR3fbZETwVjdGvBC6Xl6mY/Qn+40lMOgzPevpOtsOHJbw3PZ7TP56PA7WCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"157895361f8a2d2eec292608ed2037dfbf03d2c85e3d0f0f6eb3aafc03a08600","last_reissued_at":"2026-07-05T00:17:04.536519Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:17:04.536519Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Extended supersymmetry with central charges in Dirac action with curved extra dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","quant-ph"],"primary_cat":"hep-th","authors_text":"Inori Ueba","submitted_at":"2019-05-28T08:28:50Z","abstract_excerpt":"We discuss a new realization of $\\mathcal{N}$-extended quantum-mechanical supersymmetry (QM SUSY) with central charges hidden in the four-dimensional (4D) mass spectrum of higher dimensional Dirac action with curved extra dimensions. We show that this $\\mathcal{N}$-extended QM SUSY results from symmetries in extra dimensions, and the supermultiplets in this supersymmetry algebra correspond to the Bogomol'nyi--Prasad--Sommerfield states. Furthermore, we examine the model of the $S^2$ extra dimension with a magnetic monopole background and confirm that the $\\mathcal{N}$-extended QM SUSY explains"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1905.11673","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/1905.11673/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":"1905.11673","created_at":"2026-07-05T00:17:04.536581+00:00"},{"alias_kind":"arxiv_version","alias_value":"1905.11673v2","created_at":"2026-07-05T00:17:04.536581+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1905.11673","created_at":"2026-07-05T00:17:04.536581+00:00"},{"alias_kind":"pith_short_12","alias_value":"CV4JKNQ7RIWS","created_at":"2026-07-05T00:17:04.536581+00:00"},{"alias_kind":"pith_short_16","alias_value":"CV4JKNQ7RIWS53BJ","created_at":"2026-07-05T00:17:04.536581+00:00"},{"alias_kind":"pith_short_8","alias_value":"CV4JKNQ7","created_at":"2026-07-05T00:17:04.536581+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2505.19829","citing_title":"Gauge symmetry breaking with $S^2$ extra dimensions","ref_index":48,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CV4JKNQ7RIWS53BJEYEO2IBX36","json":"https://pith.science/pith/CV4JKNQ7RIWS53BJEYEO2IBX36.json","graph_json":"https://pith.science/api/pith-number/CV4JKNQ7RIWS53BJEYEO2IBX36/graph.json","events_json":"https://pith.science/api/pith-number/CV4JKNQ7RIWS53BJEYEO2IBX36/events.json","paper":"https://pith.science/paper/CV4JKNQ7"},"agent_actions":{"view_html":"https://pith.science/pith/CV4JKNQ7RIWS53BJEYEO2IBX36","download_json":"https://pith.science/pith/CV4JKNQ7RIWS53BJEYEO2IBX36.json","view_paper":"https://pith.science/paper/CV4JKNQ7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1905.11673&json=true","fetch_graph":"https://pith.science/api/pith-number/CV4JKNQ7RIWS53BJEYEO2IBX36/graph.json","fetch_events":"https://pith.science/api/pith-number/CV4JKNQ7RIWS53BJEYEO2IBX36/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CV4JKNQ7RIWS53BJEYEO2IBX36/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CV4JKNQ7RIWS53BJEYEO2IBX36/action/storage_attestation","attest_author":"https://pith.science/pith/CV4JKNQ7RIWS53BJEYEO2IBX36/action/author_attestation","sign_citation":"https://pith.science/pith/CV4JKNQ7RIWS53BJEYEO2IBX36/action/citation_signature","submit_replication":"https://pith.science/pith/CV4JKNQ7RIWS53BJEYEO2IBX36/action/replication_record"}},"created_at":"2026-07-05T00:17:04.536581+00:00","updated_at":"2026-07-05T00:17:04.536581+00:00"}