{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:XJEDPWBZLOLBUJTZVL3KKBS4E6","short_pith_number":"pith:XJEDPWBZ","schema_version":"1.0","canonical_sha256":"ba4837d8395b961a2679aaf6a5065c2797462a551018695d22ae8d81673bb3e3","source":{"kind":"arxiv","id":"1808.02839","version":4},"attestation_state":"computed","paper":{"title":"Nonadiabatic geometric quantum computation with parametrically tunable coupling","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"quant-ph","authors_text":"Tao Chen, Zheng-Yuan Xue","submitted_at":"2018-08-08T15:53:02Z","abstract_excerpt":"The nonadiabatic geometric quantum computation is promising as it is robust against certain types of local noises. However, its experimental implementation is challenging due to the need of complex control on multi-level and/or multiple quantum systems. Here, we propose to implement it on a two-dimensional square superconducting qubit lattice. In the construction of our geometric quantum gates, we only use the simplest and experimentally accessible control over the qubit states of the involved quantum systems, without introducing any auxiliary state. Specifically, our scheme is achieved by par"},"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":"1808.02839","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2018-08-08T15:53:02Z","cross_cats_sorted":["cond-mat.supr-con"],"title_canon_sha256":"a0236e61a17c7d658b8a8532be2b9f5e4c2f6798e7a33219047b987961e008a1","abstract_canon_sha256":"b03f0bd5ba3fd2a0e21e36dad2dd7f561eb7b2394408af0f685967ea438e8850"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:59:51.950436Z","signature_b64":"tlmnVv3myFi1bEXpfbpUd4nzWUhhy2IklHqUJ/M/q6BqbxhbSe3zmwlMB8gWm29qhZFc0WpluO8E2jNc9FlKDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ba4837d8395b961a2679aaf6a5065c2797462a551018695d22ae8d81673bb3e3","last_reissued_at":"2026-05-17T23:59:51.949983Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:59:51.949983Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nonadiabatic geometric quantum computation with parametrically tunable coupling","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"quant-ph","authors_text":"Tao Chen, Zheng-Yuan Xue","submitted_at":"2018-08-08T15:53:02Z","abstract_excerpt":"The nonadiabatic geometric quantum computation is promising as it is robust against certain types of local noises. However, its experimental implementation is challenging due to the need of complex control on multi-level and/or multiple quantum systems. Here, we propose to implement it on a two-dimensional square superconducting qubit lattice. In the construction of our geometric quantum gates, we only use the simplest and experimentally accessible control over the qubit states of the involved quantum systems, without introducing any auxiliary state. Specifically, our scheme is achieved by par"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1808.02839","kind":"arxiv","version":4},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"1808.02839","created_at":"2026-05-17T23:59:51.950057+00:00"},{"alias_kind":"arxiv_version","alias_value":"1808.02839v4","created_at":"2026-05-17T23:59:51.950057+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1808.02839","created_at":"2026-05-17T23:59:51.950057+00:00"},{"alias_kind":"pith_short_12","alias_value":"XJEDPWBZLOLB","created_at":"2026-05-18T12:33:01.666342+00:00"},{"alias_kind":"pith_short_16","alias_value":"XJEDPWBZLOLBUJTZ","created_at":"2026-05-18T12:33:01.666342+00:00"},{"alias_kind":"pith_short_8","alias_value":"XJEDPWBZ","created_at":"2026-05-18T12:33:01.666342+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/XJEDPWBZLOLBUJTZVL3KKBS4E6","json":"https://pith.science/pith/XJEDPWBZLOLBUJTZVL3KKBS4E6.json","graph_json":"https://pith.science/api/pith-number/XJEDPWBZLOLBUJTZVL3KKBS4E6/graph.json","events_json":"https://pith.science/api/pith-number/XJEDPWBZLOLBUJTZVL3KKBS4E6/events.json","paper":"https://pith.science/paper/XJEDPWBZ"},"agent_actions":{"view_html":"https://pith.science/pith/XJEDPWBZLOLBUJTZVL3KKBS4E6","download_json":"https://pith.science/pith/XJEDPWBZLOLBUJTZVL3KKBS4E6.json","view_paper":"https://pith.science/paper/XJEDPWBZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1808.02839&json=true","fetch_graph":"https://pith.science/api/pith-number/XJEDPWBZLOLBUJTZVL3KKBS4E6/graph.json","fetch_events":"https://pith.science/api/pith-number/XJEDPWBZLOLBUJTZVL3KKBS4E6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XJEDPWBZLOLBUJTZVL3KKBS4E6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XJEDPWBZLOLBUJTZVL3KKBS4E6/action/storage_attestation","attest_author":"https://pith.science/pith/XJEDPWBZLOLBUJTZVL3KKBS4E6/action/author_attestation","sign_citation":"https://pith.science/pith/XJEDPWBZLOLBUJTZVL3KKBS4E6/action/citation_signature","submit_replication":"https://pith.science/pith/XJEDPWBZLOLBUJTZVL3KKBS4E6/action/replication_record"}},"created_at":"2026-05-17T23:59:51.950057+00:00","updated_at":"2026-05-17T23:59:51.950057+00:00"}