{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:33KN6R5RSBH4YHP3I2MHSYJCK6","short_pith_number":"pith:33KN6R5R","schema_version":"1.0","canonical_sha256":"ded4df47b1904fcc1dfb46987961225789716c162b43105e76f25077baee1963","source":{"kind":"arxiv","id":"2409.03482","version":1},"attestation_state":"computed","paper":{"title":"Generating arbitrary superpositions of nonclassical quantum harmonic oscillator states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"quant-ph","authors_text":"C. J. Ballance, D. J. Webb, D. M. Lucas, G. Araneda, O. B\\u{a}z\\u{a}van, R. Srinivas, S. Saner","submitted_at":"2024-09-05T12:45:57Z","abstract_excerpt":"Full coherent control and generation of superpositions of the quantum harmonic oscillator are not only of fundamental interest but are crucial for applications in quantum simulations, quantum-enhanced metrology and continuous-variable quantum computation. The extension of such superpositions to nonclassical states increases their power as a resource for such applications. Here, we create arbitrary superpositions of nonclassical and non-Gaussian states of a quantum harmonic oscillator using the motion of a trapped ion coupled to its internal spin states. We interleave spin-dependent nonlinear b"},"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":"2409.03482","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2024-09-05T12:45:57Z","cross_cats_sorted":["physics.atom-ph"],"title_canon_sha256":"a54f896e37c92451f20e36eb2eec087343f1d36115575c3a48ac4cf27bd8a7b0","abstract_canon_sha256":"60ca0d5e3e856654b853ed2b01e88bd0a5a811c3f9aaff72971044cc337144e1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:03:32.066441Z","signature_b64":"mVmdoyyVSRXgzxhtYIUmNWUJ3IfWWjaxHCA9gkCXiza3GEoy9vrf9/UBD71b5KYQD9+XRbIkF0MWyg3GzyjwDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ded4df47b1904fcc1dfb46987961225789716c162b43105e76f25077baee1963","last_reissued_at":"2026-07-05T09:03:32.065945Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:03:32.065945Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Generating arbitrary superpositions of nonclassical quantum harmonic oscillator states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"quant-ph","authors_text":"C. J. Ballance, D. J. Webb, D. M. Lucas, G. Araneda, O. B\\u{a}z\\u{a}van, R. Srinivas, S. Saner","submitted_at":"2024-09-05T12:45:57Z","abstract_excerpt":"Full coherent control and generation of superpositions of the quantum harmonic oscillator are not only of fundamental interest but are crucial for applications in quantum simulations, quantum-enhanced metrology and continuous-variable quantum computation. The extension of such superpositions to nonclassical states increases their power as a resource for such applications. Here, we create arbitrary superpositions of nonclassical and non-Gaussian states of a quantum harmonic oscillator using the motion of a trapped ion coupled to its internal spin states. We interleave spin-dependent nonlinear b"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2409.03482","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/2409.03482/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":"2409.03482","created_at":"2026-07-05T09:03:32.066006+00:00"},{"alias_kind":"arxiv_version","alias_value":"2409.03482v1","created_at":"2026-07-05T09:03:32.066006+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2409.03482","created_at":"2026-07-05T09:03:32.066006+00:00"},{"alias_kind":"pith_short_12","alias_value":"33KN6R5RSBH4","created_at":"2026-07-05T09:03:32.066006+00:00"},{"alias_kind":"pith_short_16","alias_value":"33KN6R5RSBH4YHP3","created_at":"2026-07-05T09:03:32.066006+00:00"},{"alias_kind":"pith_short_8","alias_value":"33KN6R5R","created_at":"2026-07-05T09:03:32.066006+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.12060","citing_title":"The quantum harmonic oscillator and the real Hilbert space","ref_index":37,"is_internal_anchor":false},{"citing_arxiv_id":"2604.09958","citing_title":"Quantum metrological advantage of high-order squeezed states","ref_index":30,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/33KN6R5RSBH4YHP3I2MHSYJCK6","json":"https://pith.science/pith/33KN6R5RSBH4YHP3I2MHSYJCK6.json","graph_json":"https://pith.science/api/pith-number/33KN6R5RSBH4YHP3I2MHSYJCK6/graph.json","events_json":"https://pith.science/api/pith-number/33KN6R5RSBH4YHP3I2MHSYJCK6/events.json","paper":"https://pith.science/paper/33KN6R5R"},"agent_actions":{"view_html":"https://pith.science/pith/33KN6R5RSBH4YHP3I2MHSYJCK6","download_json":"https://pith.science/pith/33KN6R5RSBH4YHP3I2MHSYJCK6.json","view_paper":"https://pith.science/paper/33KN6R5R","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2409.03482&json=true","fetch_graph":"https://pith.science/api/pith-number/33KN6R5RSBH4YHP3I2MHSYJCK6/graph.json","fetch_events":"https://pith.science/api/pith-number/33KN6R5RSBH4YHP3I2MHSYJCK6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/33KN6R5RSBH4YHP3I2MHSYJCK6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/33KN6R5RSBH4YHP3I2MHSYJCK6/action/storage_attestation","attest_author":"https://pith.science/pith/33KN6R5RSBH4YHP3I2MHSYJCK6/action/author_attestation","sign_citation":"https://pith.science/pith/33KN6R5RSBH4YHP3I2MHSYJCK6/action/citation_signature","submit_replication":"https://pith.science/pith/33KN6R5RSBH4YHP3I2MHSYJCK6/action/replication_record"}},"created_at":"2026-07-05T09:03:32.066006+00:00","updated_at":"2026-07-05T09:03:32.066006+00:00"}