{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:LSUKPV4BO5NCHXFBUWDXMDWBLH","short_pith_number":"pith:LSUKPV4B","schema_version":"1.0","canonical_sha256":"5ca8a7d781775a23dca1a587760ec159fb64c8ebb3605b8deac50a5adf2a539f","source":{"kind":"arxiv","id":"2012.12423","version":1},"attestation_state":"computed","paper":{"title":"Sensor-assisted fault mitigation in quantum computation","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Ben Loer, John L. Orrell","submitted_at":"2020-12-23T00:17:32Z","abstract_excerpt":"We propose a method to assist fault mitigation in quantum computation through the use of sensors co-located near physical qubits. Specifically, we consider using transition edge sensors co-located on silicon substrates hosting superconducting qubits to monitor for energy injection from ionizing radiation, which has been demonstrated to increase decoherence in transmon qubits. We generalize from these two physical device concepts and explore the potential advantages of co-located sensors to assist fault mitigation in quantum computation. In the simplest scheme, co-located sensors beneficially 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":"2012.12423","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"quant-ph","submitted_at":"2020-12-23T00:17:32Z","cross_cats_sorted":[],"title_canon_sha256":"8abfc04f2f9acbb4aeac770037a1c699ddb94e218983a4728a75590af754a0cb","abstract_canon_sha256":"45d2e36b36de0ca21d186a2137c0daa063d9d957fa4e542212159b8a520efd06"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:09:28.589745Z","signature_b64":"BTUyH/qvLvx2UHdKJWDu52NK7rGxaWt7gZhnlSu8+a/9PubOaZXhBwjvMpWqS6+u5F9lvUQnHUshx9hGyBdTBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5ca8a7d781775a23dca1a587760ec159fb64c8ebb3605b8deac50a5adf2a539f","last_reissued_at":"2026-07-05T03:09:28.589327Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:09:28.589327Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Sensor-assisted fault mitigation in quantum computation","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Ben Loer, John L. Orrell","submitted_at":"2020-12-23T00:17:32Z","abstract_excerpt":"We propose a method to assist fault mitigation in quantum computation through the use of sensors co-located near physical qubits. Specifically, we consider using transition edge sensors co-located on silicon substrates hosting superconducting qubits to monitor for energy injection from ionizing radiation, which has been demonstrated to increase decoherence in transmon qubits. We generalize from these two physical device concepts and explore the potential advantages of co-located sensors to assist fault mitigation in quantum computation. In the simplest scheme, co-located sensors beneficially a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2012.12423","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/2012.12423/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":"2012.12423","created_at":"2026-07-05T03:09:28.589384+00:00"},{"alias_kind":"arxiv_version","alias_value":"2012.12423v1","created_at":"2026-07-05T03:09:28.589384+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2012.12423","created_at":"2026-07-05T03:09:28.589384+00:00"},{"alias_kind":"pith_short_12","alias_value":"LSUKPV4BO5NC","created_at":"2026-07-05T03:09:28.589384+00:00"},{"alias_kind":"pith_short_16","alias_value":"LSUKPV4BO5NCHXFB","created_at":"2026-07-05T03:09:28.589384+00:00"},{"alias_kind":"pith_short_8","alias_value":"LSUKPV4B","created_at":"2026-07-05T03:09:28.589384+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.13176","citing_title":"Measuring quasiparticle dynamics for particle impact reconstruction in a superconducting qubit chip","ref_index":35,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LSUKPV4BO5NCHXFBUWDXMDWBLH","json":"https://pith.science/pith/LSUKPV4BO5NCHXFBUWDXMDWBLH.json","graph_json":"https://pith.science/api/pith-number/LSUKPV4BO5NCHXFBUWDXMDWBLH/graph.json","events_json":"https://pith.science/api/pith-number/LSUKPV4BO5NCHXFBUWDXMDWBLH/events.json","paper":"https://pith.science/paper/LSUKPV4B"},"agent_actions":{"view_html":"https://pith.science/pith/LSUKPV4BO5NCHXFBUWDXMDWBLH","download_json":"https://pith.science/pith/LSUKPV4BO5NCHXFBUWDXMDWBLH.json","view_paper":"https://pith.science/paper/LSUKPV4B","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2012.12423&json=true","fetch_graph":"https://pith.science/api/pith-number/LSUKPV4BO5NCHXFBUWDXMDWBLH/graph.json","fetch_events":"https://pith.science/api/pith-number/LSUKPV4BO5NCHXFBUWDXMDWBLH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LSUKPV4BO5NCHXFBUWDXMDWBLH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LSUKPV4BO5NCHXFBUWDXMDWBLH/action/storage_attestation","attest_author":"https://pith.science/pith/LSUKPV4BO5NCHXFBUWDXMDWBLH/action/author_attestation","sign_citation":"https://pith.science/pith/LSUKPV4BO5NCHXFBUWDXMDWBLH/action/citation_signature","submit_replication":"https://pith.science/pith/LSUKPV4BO5NCHXFBUWDXMDWBLH/action/replication_record"}},"created_at":"2026-07-05T03:09:28.589384+00:00","updated_at":"2026-07-05T03:09:28.589384+00:00"}