{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2020:QQ7UDVYPO7CAYDHN2ZPEKK63KU","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"175823b94906ce464fc8a646a20ca77e152e44c5c74bb3aeebf060c32fbf757b","cross_cats_sorted":["math-ph","math.MP","nlin.SI","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2020-02-11T12:14:38Z","title_canon_sha256":"671ead172fbb9ae7c599e2f46a99cbd13beeb84b5954388bf5f532b71ec1186e"},"schema_version":"1.0","source":{"id":"2002.04341","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2002.04341","created_at":"2026-07-05T00:54:13Z"},{"alias_kind":"arxiv_version","alias_value":"2002.04341v4","created_at":"2026-07-05T00:54:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2002.04341","created_at":"2026-07-05T00:54:13Z"},{"alias_kind":"pith_short_12","alias_value":"QQ7UDVYPO7CA","created_at":"2026-07-05T00:54:13Z"},{"alias_kind":"pith_short_16","alias_value":"QQ7UDVYPO7CAYDHN","created_at":"2026-07-05T00:54:13Z"},{"alias_kind":"pith_short_8","alias_value":"QQ7UDVYP","created_at":"2026-07-05T00:54:13Z"}],"graph_snapshots":[{"event_id":"sha256:905bcd6d6b69179caf21c553a7be0e80a7d760049cadcd22442e180538a7cac4","target":"graph","created_at":"2026-07-05T00:54:13Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2002.04341/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study classical and quantum hidden symmetries of a particle with electric charge $e$ in the background of a Dirac monopole of magnetic charge $g$ subjected to an additional central potential $V(r)=U(r) +(eg)^2/2mr^{2}$ with $U(r)=\\tfrac{1}{2}m\\omega^2r^2$, similar to that in the one-dimensional conformal mechanics model of de Alfaro, Fubini and Furlan (AFF). By means of a non-unitary conformal bridge transformation, we establish a relation of the quantum states and of all symmetries of the system with those of the system without harmonic trap, $U(r)=0$. Introducing spin degrees of freedom v","authors_text":"Andreas Wipf, Luis Inzunza, Mikhail S. Plyushchay","cross_cats":["math-ph","math.MP","nlin.SI","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2020-02-11T12:14:38Z","title":"Hidden symmetry and (super)conformal mechanics in a monopole background"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2002.04341","kind":"arxiv","version":4},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:1f7b8e1fb239df17ac49b15c673d4787c75838181cef06bbac386369bfc1a35f","target":"record","created_at":"2026-07-05T00:54:13Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"175823b94906ce464fc8a646a20ca77e152e44c5c74bb3aeebf060c32fbf757b","cross_cats_sorted":["math-ph","math.MP","nlin.SI","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2020-02-11T12:14:38Z","title_canon_sha256":"671ead172fbb9ae7c599e2f46a99cbd13beeb84b5954388bf5f532b71ec1186e"},"schema_version":"1.0","source":{"id":"2002.04341","kind":"arxiv","version":4}},"canonical_sha256":"843f41d70f77c40c0cedd65e452bdb5511ee6cdc3f5ea83ad1c8a6f585ffa6ea","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"843f41d70f77c40c0cedd65e452bdb5511ee6cdc3f5ea83ad1c8a6f585ffa6ea","first_computed_at":"2026-07-05T00:54:13.010712Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T00:54:13.010712Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"LY9qHbhnncVWnp4LpcXhIMspTNRWeeF460mSdl35MFHuPEmkCamp3nn3/10+/um3uYj90EdmH0lO2MZGHWa6AA==","signature_status":"signed_v1","signed_at":"2026-07-05T00:54:13.011249Z","signed_message":"canonical_sha256_bytes"},"source_id":"2002.04341","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1f7b8e1fb239df17ac49b15c673d4787c75838181cef06bbac386369bfc1a35f","sha256:905bcd6d6b69179caf21c553a7be0e80a7d760049cadcd22442e180538a7cac4"],"state_sha256":"7df3cff24ab09ba537514699e2f6a4dadd2a0058547c95792946d0eb0c4643eb"}