{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:7GAA72LCFDWFB4U3H5XEFMWX7X","short_pith_number":"pith:7GAA72LC","schema_version":"1.0","canonical_sha256":"f9800fe96228ec50f29b3f6e42b2d7fdff858d701c128789a85304cdafe58ef9","source":{"kind":"arxiv","id":"2607.21360","version":1},"attestation_state":"computed","paper":{"title":"Floquet Reservoir Engineering for Remote Logical Entanglement","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Aashish A. Clerk, Mingxing Yao","submitted_at":"2026-07-23T14:23:24Z","abstract_excerpt":"Implementing controlled dissipative dynamics is a powerful approach for state preparation in a variety of contexts, including the preparation of remote entangled states. Here, we show that by going beyond the standard setting of time-independent dissipative dynamics, one can realize even more powerful non-unitary protocols. We introduce dissipative Floquet protocols for stabilizing remote entanglement of logical qubits, where continuously-running dissipation is interleaved with a periodic sequence of unitary gates. These protocols harness existing experimental capabilities, and overcome time-e"},"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":"2607.21360","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2026-07-23T14:23:24Z","cross_cats_sorted":[],"title_canon_sha256":"05e3cadbe8903bec01cb51e6140321f62d423739ff1cbe3e758f0a418421c284","abstract_canon_sha256":"674bfca75a7e71e3cc0c615a36578e135f41da5a82ef1479cc82bff49db857a0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-24T01:24:27.492783Z","signature_b64":"2UoLYOd46cHJQArPS4npszhWvCYl8uoKRbqJjNsDBBUuMJpWuEP4Zs/TdKqQ6Fj728Bo23Q7KybJ61YE6iACCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f9800fe96228ec50f29b3f6e42b2d7fdff858d701c128789a85304cdafe58ef9","last_reissued_at":"2026-07-24T01:24:27.491889Z","signature_status":"signed_v1","first_computed_at":"2026-07-24T01:24:27.491889Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Floquet Reservoir Engineering for Remote Logical Entanglement","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Aashish A. Clerk, Mingxing Yao","submitted_at":"2026-07-23T14:23:24Z","abstract_excerpt":"Implementing controlled dissipative dynamics is a powerful approach for state preparation in a variety of contexts, including the preparation of remote entangled states. Here, we show that by going beyond the standard setting of time-independent dissipative dynamics, one can realize even more powerful non-unitary protocols. We introduce dissipative Floquet protocols for stabilizing remote entanglement of logical qubits, where continuously-running dissipation is interleaved with a periodic sequence of unitary gates. These protocols harness existing experimental capabilities, and overcome time-e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.21360","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/2607.21360/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":"2607.21360","created_at":"2026-07-24T01:24:27.492341+00:00"},{"alias_kind":"arxiv_version","alias_value":"2607.21360v1","created_at":"2026-07-24T01:24:27.492341+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.21360","created_at":"2026-07-24T01:24:27.492341+00:00"},{"alias_kind":"pith_short_12","alias_value":"7GAA72LCFDWF","created_at":"2026-07-24T01:24:27.492341+00:00"},{"alias_kind":"pith_short_16","alias_value":"7GAA72LCFDWFB4U3","created_at":"2026-07-24T01:24:27.492341+00:00"},{"alias_kind":"pith_short_8","alias_value":"7GAA72LC","created_at":"2026-07-24T01:24:27.492341+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2608.08346","citing_title":"Entanglement and non-local magic in a non-unitarily deformed non-Hermitian bipartite system","ref_index":36,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7GAA72LCFDWFB4U3H5XEFMWX7X","json":"https://pith.science/pith/7GAA72LCFDWFB4U3H5XEFMWX7X.json","graph_json":"https://pith.science/api/pith-number/7GAA72LCFDWFB4U3H5XEFMWX7X/graph.json","events_json":"https://pith.science/api/pith-number/7GAA72LCFDWFB4U3H5XEFMWX7X/events.json","paper":"https://pith.science/paper/7GAA72LC"},"agent_actions":{"view_html":"https://pith.science/pith/7GAA72LCFDWFB4U3H5XEFMWX7X","download_json":"https://pith.science/pith/7GAA72LCFDWFB4U3H5XEFMWX7X.json","view_paper":"https://pith.science/paper/7GAA72LC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2607.21360&json=true","fetch_graph":"https://pith.science/api/pith-number/7GAA72LCFDWFB4U3H5XEFMWX7X/graph.json","fetch_events":"https://pith.science/api/pith-number/7GAA72LCFDWFB4U3H5XEFMWX7X/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7GAA72LCFDWFB4U3H5XEFMWX7X/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7GAA72LCFDWFB4U3H5XEFMWX7X/action/storage_attestation","attest_author":"https://pith.science/pith/7GAA72LCFDWFB4U3H5XEFMWX7X/action/author_attestation","sign_citation":"https://pith.science/pith/7GAA72LCFDWFB4U3H5XEFMWX7X/action/citation_signature","submit_replication":"https://pith.science/pith/7GAA72LCFDWFB4U3H5XEFMWX7X/action/replication_record"}},"created_at":"2026-07-24T01:24:27.492341+00:00","updated_at":"2026-07-24T01:24:27.492341+00:00"}