{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:7P6IQA3ELRV3XJDSTTAVQ3WQMN","short_pith_number":"pith:7P6IQA3E","schema_version":"1.0","canonical_sha256":"fbfc8803645c6bbba4729cc1586ed063559e629e7d7424b64c2521deb23d81cd","source":{"kind":"arxiv","id":"2606.18755","version":1},"attestation_state":"computed","paper":{"title":"Quantum simulation of neutrino oscillations with bosonic encoding","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"quant-ph","authors_text":"Sandeep Joshi","submitted_at":"2026-06-17T07:01:20Z","abstract_excerpt":"Superconducting qubits offer a versatile platform for quantum simulation. In this architecture, quantum information can be encoded in the bosonic modes of a microwave cavity, offering an alternative to conventional qubit-based encoding schemes. These cavity bosonic modes can be manipulated using a single ancillary qubit. In this work, we investigate the quantum simulation of two- and three-flavor neutrino oscillations using Fock-basis encoding of a cavity mode. We design pulse sequences for implementing the required unitary operations through selective number-dependent arbitrary phase (SNAP) a"},"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":"2606.18755","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2026-06-17T07:01:20Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"88c0f56c03790e0a94d22057f4006bade4bff62089ff4dc74fb95e993024b7dd","abstract_canon_sha256":"ed7631442724cb872438b7356675ac2d5815720339ac1fde601df6b2eb9f35f7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-19T16:11:46.556921Z","signature_b64":"rI4qfr17CbgoaD0pBo8l14H895T/dKbpqLaFTVb85/xck34Alr0uW3m62C5uhGenQmaJ9Q/QWItsZumKV0wIAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fbfc8803645c6bbba4729cc1586ed063559e629e7d7424b64c2521deb23d81cd","last_reissued_at":"2026-06-19T16:11:46.556572Z","signature_status":"signed_v1","first_computed_at":"2026-06-19T16:11:46.556572Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum simulation of neutrino oscillations with bosonic encoding","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"quant-ph","authors_text":"Sandeep Joshi","submitted_at":"2026-06-17T07:01:20Z","abstract_excerpt":"Superconducting qubits offer a versatile platform for quantum simulation. In this architecture, quantum information can be encoded in the bosonic modes of a microwave cavity, offering an alternative to conventional qubit-based encoding schemes. These cavity bosonic modes can be manipulated using a single ancillary qubit. In this work, we investigate the quantum simulation of two- and three-flavor neutrino oscillations using Fock-basis encoding of a cavity mode. We design pulse sequences for implementing the required unitary operations through selective number-dependent arbitrary phase (SNAP) a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.18755","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/2606.18755/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":"2606.18755","created_at":"2026-06-19T16:11:46.556634+00:00"},{"alias_kind":"arxiv_version","alias_value":"2606.18755v1","created_at":"2026-06-19T16:11:46.556634+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.18755","created_at":"2026-06-19T16:11:46.556634+00:00"},{"alias_kind":"pith_short_12","alias_value":"7P6IQA3ELRV3","created_at":"2026-06-19T16:11:46.556634+00:00"},{"alias_kind":"pith_short_16","alias_value":"7P6IQA3ELRV3XJDS","created_at":"2026-06-19T16:11:46.556634+00:00"},{"alias_kind":"pith_short_8","alias_value":"7P6IQA3E","created_at":"2026-06-19T16:11:46.556634+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/7P6IQA3ELRV3XJDSTTAVQ3WQMN","json":"https://pith.science/pith/7P6IQA3ELRV3XJDSTTAVQ3WQMN.json","graph_json":"https://pith.science/api/pith-number/7P6IQA3ELRV3XJDSTTAVQ3WQMN/graph.json","events_json":"https://pith.science/api/pith-number/7P6IQA3ELRV3XJDSTTAVQ3WQMN/events.json","paper":"https://pith.science/paper/7P6IQA3E"},"agent_actions":{"view_html":"https://pith.science/pith/7P6IQA3ELRV3XJDSTTAVQ3WQMN","download_json":"https://pith.science/pith/7P6IQA3ELRV3XJDSTTAVQ3WQMN.json","view_paper":"https://pith.science/paper/7P6IQA3E","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2606.18755&json=true","fetch_graph":"https://pith.science/api/pith-number/7P6IQA3ELRV3XJDSTTAVQ3WQMN/graph.json","fetch_events":"https://pith.science/api/pith-number/7P6IQA3ELRV3XJDSTTAVQ3WQMN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7P6IQA3ELRV3XJDSTTAVQ3WQMN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7P6IQA3ELRV3XJDSTTAVQ3WQMN/action/storage_attestation","attest_author":"https://pith.science/pith/7P6IQA3ELRV3XJDSTTAVQ3WQMN/action/author_attestation","sign_citation":"https://pith.science/pith/7P6IQA3ELRV3XJDSTTAVQ3WQMN/action/citation_signature","submit_replication":"https://pith.science/pith/7P6IQA3ELRV3XJDSTTAVQ3WQMN/action/replication_record"}},"created_at":"2026-06-19T16:11:46.556634+00:00","updated_at":"2026-06-19T16:11:46.556634+00:00"}