{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:XN4HYI4IVGKJ4DF3EAEVK55UDW","short_pith_number":"pith:XN4HYI4I","schema_version":"1.0","canonical_sha256":"bb787c2388a9949e0cbb20095577b41d9e255b64c398d56ee04602945655ee78","source":{"kind":"arxiv","id":"1511.01760","version":1},"attestation_state":"computed","paper":{"title":"High Kinetic Inductance Superconducting Nanowire Resonators for Circuit QED in a Magnetic Field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"A. Bruno, D. P. DiVincenzo, G. Zheng, L. DiCarlo, L. M. K. Vandersypen, N. Samkharadze, P. Scarlino","submitted_at":"2015-11-05T14:30:22Z","abstract_excerpt":"We present superconducting microwave-frequency resonators based on NbTiN nanowires. The small cross section of the nanowires minimizes vortex generation, making the resonators resilient to magnetic fields. Measured intrinsic quality factors exceed $2\\times 10^5$ in a $6$ T in-plane magnetic field, and $3\\times 10^4$ in a $350$ mT perpendicular magnetic field. Due to their high characteristic impedance, these resonators are expected to develop zero-point voltage fluctuations one order of magnitude larger than in standard coplanar waveguide resonators. These properties make the nanowire resonato"},"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":"1511.01760","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-11-05T14:30:22Z","cross_cats_sorted":[],"title_canon_sha256":"8b31d42b37254c9b3bb4d854c59c21ea7a669c77b6998dbda97da673cf3b268e","abstract_canon_sha256":"6dc3bdefb9d20e09710af3c09712035b9799b95b968a58366a6daec7a53f5560"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:17:18.447081Z","signature_b64":"a4kOpyFVAWJnImV2nkHskIRhqlLxpMXwRFfkIOhEoPR4t4wFupBupHrCpXOmwfRZSAtg4G8eZuiH1HFARqVNBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bb787c2388a9949e0cbb20095577b41d9e255b64c398d56ee04602945655ee78","last_reissued_at":"2026-05-18T01:17:18.446648Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:17:18.446648Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"High Kinetic Inductance Superconducting Nanowire Resonators for Circuit QED in a Magnetic Field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"A. Bruno, D. P. DiVincenzo, G. Zheng, L. DiCarlo, L. M. K. Vandersypen, N. Samkharadze, P. Scarlino","submitted_at":"2015-11-05T14:30:22Z","abstract_excerpt":"We present superconducting microwave-frequency resonators based on NbTiN nanowires. The small cross section of the nanowires minimizes vortex generation, making the resonators resilient to magnetic fields. Measured intrinsic quality factors exceed $2\\times 10^5$ in a $6$ T in-plane magnetic field, and $3\\times 10^4$ in a $350$ mT perpendicular magnetic field. Due to their high characteristic impedance, these resonators are expected to develop zero-point voltage fluctuations one order of magnitude larger than in standard coplanar waveguide resonators. These properties make the nanowire resonato"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.01760","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":""},"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":"1511.01760","created_at":"2026-05-18T01:17:18.446721+00:00"},{"alias_kind":"arxiv_version","alias_value":"1511.01760v1","created_at":"2026-05-18T01:17:18.446721+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.01760","created_at":"2026-05-18T01:17:18.446721+00:00"},{"alias_kind":"pith_short_12","alias_value":"XN4HYI4IVGKJ","created_at":"2026-05-18T12:29:50.041715+00:00"},{"alias_kind":"pith_short_16","alias_value":"XN4HYI4IVGKJ4DF3","created_at":"2026-05-18T12:29:50.041715+00:00"},{"alias_kind":"pith_short_8","alias_value":"XN4HYI4I","created_at":"2026-05-18T12:29:50.041715+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/XN4HYI4IVGKJ4DF3EAEVK55UDW","json":"https://pith.science/pith/XN4HYI4IVGKJ4DF3EAEVK55UDW.json","graph_json":"https://pith.science/api/pith-number/XN4HYI4IVGKJ4DF3EAEVK55UDW/graph.json","events_json":"https://pith.science/api/pith-number/XN4HYI4IVGKJ4DF3EAEVK55UDW/events.json","paper":"https://pith.science/paper/XN4HYI4I"},"agent_actions":{"view_html":"https://pith.science/pith/XN4HYI4IVGKJ4DF3EAEVK55UDW","download_json":"https://pith.science/pith/XN4HYI4IVGKJ4DF3EAEVK55UDW.json","view_paper":"https://pith.science/paper/XN4HYI4I","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1511.01760&json=true","fetch_graph":"https://pith.science/api/pith-number/XN4HYI4IVGKJ4DF3EAEVK55UDW/graph.json","fetch_events":"https://pith.science/api/pith-number/XN4HYI4IVGKJ4DF3EAEVK55UDW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XN4HYI4IVGKJ4DF3EAEVK55UDW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XN4HYI4IVGKJ4DF3EAEVK55UDW/action/storage_attestation","attest_author":"https://pith.science/pith/XN4HYI4IVGKJ4DF3EAEVK55UDW/action/author_attestation","sign_citation":"https://pith.science/pith/XN4HYI4IVGKJ4DF3EAEVK55UDW/action/citation_signature","submit_replication":"https://pith.science/pith/XN4HYI4IVGKJ4DF3EAEVK55UDW/action/replication_record"}},"created_at":"2026-05-18T01:17:18.446721+00:00","updated_at":"2026-05-18T01:17:18.446721+00:00"}