{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:LKZEVYEBOW5DMGFAPCTTMKLEZU","short_pith_number":"pith:LKZEVYEB","schema_version":"1.0","canonical_sha256":"5ab24ae08175ba3618a078a7362964cd2807e1e4e296d8e3f705b890b2400cdd","source":{"kind":"arxiv","id":"1701.03433","version":1},"attestation_state":"computed","paper":{"title":"Strong Coupling Cavity QED with Gate-Defined Double Quantum Dots Enabled by a High Impedance Resonator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"Andreas Wallraff, Anna Stockklauser, Christian Kraglund Andersen, Christian Reichl, Jonne Koski, Klaus Ensslin, Pasquale Scarlino, Simone Gasparinetti, Thomas Ihn, Werner Wegscheider","submitted_at":"2017-01-12T17:47:12Z","abstract_excerpt":"The strong coupling limit of cavity quantum electrodynamics (QED) implies the capability of a matter-like quantum system to coherently transform an individual excitation into a single photon within a resonant structure. This not only enables essential processes required for quantum information processing but also allows for fundamental studies of matter-light interaction. In this work we demonstrate strong coupling between the charge degree of freedom in a gate-detuned GaAs double quantum dot (DQD) and a frequency-tunable high impedance resonator realized using an array of superconducting quan"},"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":"1701.03433","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-01-12T17:47:12Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"83230c6487ba99960ec81e85f68ae65b8440542f6485e057a0df0197d921d7b0","abstract_canon_sha256":"5f1d53997d792b743510f6800830c139e980a10224a8f644bbd2f3134353327d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:48:15.385148Z","signature_b64":"mHaWeVsf49/lDNADdEERe+/AwakwqBH82GpCsIItMBs9h62ZMx4/ZiY1li1v3xjf4kej/qARN7PvPypBznjiDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5ab24ae08175ba3618a078a7362964cd2807e1e4e296d8e3f705b890b2400cdd","last_reissued_at":"2026-05-18T00:48:15.384404Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:48:15.384404Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Strong Coupling Cavity QED with Gate-Defined Double Quantum Dots Enabled by a High Impedance Resonator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"Andreas Wallraff, Anna Stockklauser, Christian Kraglund Andersen, Christian Reichl, Jonne Koski, Klaus Ensslin, Pasquale Scarlino, Simone Gasparinetti, Thomas Ihn, Werner Wegscheider","submitted_at":"2017-01-12T17:47:12Z","abstract_excerpt":"The strong coupling limit of cavity quantum electrodynamics (QED) implies the capability of a matter-like quantum system to coherently transform an individual excitation into a single photon within a resonant structure. This not only enables essential processes required for quantum information processing but also allows for fundamental studies of matter-light interaction. In this work we demonstrate strong coupling between the charge degree of freedom in a gate-detuned GaAs double quantum dot (DQD) and a frequency-tunable high impedance resonator realized using an array of superconducting quan"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.03433","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":"1701.03433","created_at":"2026-05-18T00:48:15.384522+00:00"},{"alias_kind":"arxiv_version","alias_value":"1701.03433v1","created_at":"2026-05-18T00:48:15.384522+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.03433","created_at":"2026-05-18T00:48:15.384522+00:00"},{"alias_kind":"pith_short_12","alias_value":"LKZEVYEBOW5D","created_at":"2026-05-18T12:31:28.150371+00:00"},{"alias_kind":"pith_short_16","alias_value":"LKZEVYEBOW5DMGFA","created_at":"2026-05-18T12:31:28.150371+00:00"},{"alias_kind":"pith_short_8","alias_value":"LKZEVYEB","created_at":"2026-05-18T12:31:28.150371+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/LKZEVYEBOW5DMGFAPCTTMKLEZU","json":"https://pith.science/pith/LKZEVYEBOW5DMGFAPCTTMKLEZU.json","graph_json":"https://pith.science/api/pith-number/LKZEVYEBOW5DMGFAPCTTMKLEZU/graph.json","events_json":"https://pith.science/api/pith-number/LKZEVYEBOW5DMGFAPCTTMKLEZU/events.json","paper":"https://pith.science/paper/LKZEVYEB"},"agent_actions":{"view_html":"https://pith.science/pith/LKZEVYEBOW5DMGFAPCTTMKLEZU","download_json":"https://pith.science/pith/LKZEVYEBOW5DMGFAPCTTMKLEZU.json","view_paper":"https://pith.science/paper/LKZEVYEB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1701.03433&json=true","fetch_graph":"https://pith.science/api/pith-number/LKZEVYEBOW5DMGFAPCTTMKLEZU/graph.json","fetch_events":"https://pith.science/api/pith-number/LKZEVYEBOW5DMGFAPCTTMKLEZU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LKZEVYEBOW5DMGFAPCTTMKLEZU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LKZEVYEBOW5DMGFAPCTTMKLEZU/action/storage_attestation","attest_author":"https://pith.science/pith/LKZEVYEBOW5DMGFAPCTTMKLEZU/action/author_attestation","sign_citation":"https://pith.science/pith/LKZEVYEBOW5DMGFAPCTTMKLEZU/action/citation_signature","submit_replication":"https://pith.science/pith/LKZEVYEBOW5DMGFAPCTTMKLEZU/action/replication_record"}},"created_at":"2026-05-18T00:48:15.384522+00:00","updated_at":"2026-05-18T00:48:15.384522+00:00"}