{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:I4YQYJCXE5WODM4V6G2EKV43EB","short_pith_number":"pith:I4YQYJCX","schema_version":"1.0","canonical_sha256":"47310c2457276ce1b395f1b445579b20608ca1dc7cc06ae02cccdea1179dc6d6","source":{"kind":"arxiv","id":"2401.09040","version":2},"attestation_state":"computed","paper":{"title":"Pseudo Twirling Mitigation of Coherent Errors in non-Clifford Gates","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Ben Bar, Jader P. Santos, Raam Uzdin","submitted_at":"2024-01-17T08:14:59Z","abstract_excerpt":"The conventional circuit paradigm, utilizing a limited number of gates to construct arbitrary quantum circuits, is hindered by significant noise overhead. For instance, the standard gate paradigm employs two CNOT gates for the partial CPhase rotation in the quantum Fourier transform, even when the rotation angle is very small. In contrast, some quantum computer platforms can directly implement such operations using their native interaction, resulting in considerably shorter and less noisy implementations for small rotation angles. Unfortunately, coherent errors stemming from qubit crosstalk an"},"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":"2401.09040","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"quant-ph","submitted_at":"2024-01-17T08:14:59Z","cross_cats_sorted":[],"title_canon_sha256":"5f115ae254be5568597b186f8e99b6f4c9325da08b7c5992e7f27fb228a0621b","abstract_canon_sha256":"49569e62d86d43f193222db1bd7861bbc18ff1089bb31adb1da72dd5b8060089"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:03:48.011533Z","signature_b64":"3H0JO6W1+H+3wtLnsFWJNH5F0cXb4gPNiweoLWAqVhVMst9PGnHYxYzuYVC04/c228lvVUWE8xx/pbm4dP2WCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"47310c2457276ce1b395f1b445579b20608ca1dc7cc06ae02cccdea1179dc6d6","last_reissued_at":"2026-07-05T08:03:48.011064Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:03:48.011064Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Pseudo Twirling Mitigation of Coherent Errors in non-Clifford Gates","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Ben Bar, Jader P. Santos, Raam Uzdin","submitted_at":"2024-01-17T08:14:59Z","abstract_excerpt":"The conventional circuit paradigm, utilizing a limited number of gates to construct arbitrary quantum circuits, is hindered by significant noise overhead. For instance, the standard gate paradigm employs two CNOT gates for the partial CPhase rotation in the quantum Fourier transform, even when the rotation angle is very small. In contrast, some quantum computer platforms can directly implement such operations using their native interaction, resulting in considerably shorter and less noisy implementations for small rotation angles. Unfortunately, coherent errors stemming from qubit crosstalk an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2401.09040","kind":"arxiv","version":2},"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/2401.09040/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":"2401.09040","created_at":"2026-07-05T08:03:48.011122+00:00"},{"alias_kind":"arxiv_version","alias_value":"2401.09040v2","created_at":"2026-07-05T08:03:48.011122+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2401.09040","created_at":"2026-07-05T08:03:48.011122+00:00"},{"alias_kind":"pith_short_12","alias_value":"I4YQYJCXE5WO","created_at":"2026-07-05T08:03:48.011122+00:00"},{"alias_kind":"pith_short_16","alias_value":"I4YQYJCXE5WODM4V","created_at":"2026-07-05T08:03:48.011122+00:00"},{"alias_kind":"pith_short_8","alias_value":"I4YQYJCX","created_at":"2026-07-05T08:03:48.011122+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.10318","citing_title":"Analysis and Suppression of Errors in Quantum Random Access Memory under Extended Noise Models","ref_index":48,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/I4YQYJCXE5WODM4V6G2EKV43EB","json":"https://pith.science/pith/I4YQYJCXE5WODM4V6G2EKV43EB.json","graph_json":"https://pith.science/api/pith-number/I4YQYJCXE5WODM4V6G2EKV43EB/graph.json","events_json":"https://pith.science/api/pith-number/I4YQYJCXE5WODM4V6G2EKV43EB/events.json","paper":"https://pith.science/paper/I4YQYJCX"},"agent_actions":{"view_html":"https://pith.science/pith/I4YQYJCXE5WODM4V6G2EKV43EB","download_json":"https://pith.science/pith/I4YQYJCXE5WODM4V6G2EKV43EB.json","view_paper":"https://pith.science/paper/I4YQYJCX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2401.09040&json=true","fetch_graph":"https://pith.science/api/pith-number/I4YQYJCXE5WODM4V6G2EKV43EB/graph.json","fetch_events":"https://pith.science/api/pith-number/I4YQYJCXE5WODM4V6G2EKV43EB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/I4YQYJCXE5WODM4V6G2EKV43EB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/I4YQYJCXE5WODM4V6G2EKV43EB/action/storage_attestation","attest_author":"https://pith.science/pith/I4YQYJCXE5WODM4V6G2EKV43EB/action/author_attestation","sign_citation":"https://pith.science/pith/I4YQYJCXE5WODM4V6G2EKV43EB/action/citation_signature","submit_replication":"https://pith.science/pith/I4YQYJCXE5WODM4V6G2EKV43EB/action/replication_record"}},"created_at":"2026-07-05T08:03:48.011122+00:00","updated_at":"2026-07-05T08:03:48.011122+00:00"}