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APS

Weak measurement of a solid-state qubit revealed in low-frequency noise

Alexander N. Korotkov

Published Mar 1, 2009• 0 citations
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Related papers

Measurement-induced qubit state mixing from upconverted low frequency noise

D. H. Slichter, Rajamani Vijay, Steve Weber +1 more

Bulletin of the American Physical Society•Mar 2, 2012•0 citations

Correcting Low-Frequency Noise with Continuous Measurement

Lin Tian

Low-frequency noise presents a serious source of decoherence in solid-state qubits. When combined with a continuous weak measurement of the eigenstates, low-frequency noise induces a second-order relaxation between the qubit states. Here, we show that the relaxation provides a unique approach to calibrate the low-frequency noise in the time domain. By encoding one qubit with two physical qubits that are alternatively calibrated, quantum-logic gates with high fidelity can be performed.

arXiv:quant-ph/0606158•Physical Review Letters•Apr 13, 2007•12 citations

QUBIT DECOHERENCE BY LOW-FREQUENCY NOISE

Kristian Rabenstein, Viktor A. Sverdlov, D. V. Averin

International Symposium on Mesoscopic Superconductivity and Spintronics (MS+S)•Aug 1, 2005•1 citation

Model for monitoring of a charge qubit using a radio-frequency quantum point contact including experimental imperfections

Neil P. Oxtoby, Jay Gambetta, Howard M. Wiseman

The extension of quantum trajectory theory to incorporate realistic imperfections in the measurement of solid-state qubits is important for quantum computation, particularly for the purposes of state preparation and error correction as well as for readout of computations. Previously this has been achieved for low-frequency (dc) weak measurements. In this paper we extend realistic quantum trajectory theory to include radio frequency (rf) weak measurements where a low-transparency quantum point contact (QPC), coupled to a charge qubit, is used to damp a classical oscillator circuit. The resulting realistic quantum trajectory equation must be solved numerically. We present an analytical result for the limit of large dissipation within the oscillator (relative to the QPC), where the oscillator slaves to the qubit. The $\mathrm{rf}+\mathrm{dc}$ mode of operation is considered. Here the QPC is biased (dc) as well as subjected to a small-amplitude sinusoidal carrier signal (rf). The $\mathrm{rf}+\mathrm{dc}$ QPC is shown to be a low-efficiency charge-qubit detector, which may nevertheless be higher than the dc-QPC (which is subject to $1∕f$ noise).

arXiv:0706.3527•Physical Review B•Mar 5, 2008•18 citations

Feedback suppression of the low-frequency noise in qubits by the low-frequency quantum measurements

Qiang Deng, D. V. Averin

Bulletin of the American Physical Society•Mar 23, 2011•0 citations

Characterising a solid state qubit via environmental noise

Jason F. Ralph, Terrence D. Clark, M. J. Everitt +3 more

arXiv:cond-mat/0306475•Physics Letters A•Sep 22, 2003•4 citations
The extension of quantum trajectory theory to incorporate realistic imperfections in the measurement of solid-state qubits is important for quantum computation, particularly for the purposes of state preparation and error correction as well as for readout of computations. Previously this has been achieved for low-frequency (dc) weak measurements. In this paper we extend realistic quantum trajectory theory to include radio frequency (rf) weak measurements where a low-transparency quantum point contact (QPC), coupled to a charge qubit, is used to damp a classical oscillator circuit. The resulting realistic quantum trajectory equation must be solved numerically. We present an analytical result for the limit of large dissipation within the oscillator (relative to the QPC), where the oscillator slaves to the qubit. The rf+dc\mathrm{rf}+\mathrm{dc}rf+dc mode of operation is considered. Here the QPC is biased (dc) as well as subjected to a small-amplitude sinusoidal carrier signal (rf). The rf+dc\mathrm{rf}+\mathrm{dc}rf+dc QPC is shown to be a low-efficiency charge-qubit detector, which may nevertheless be higher than the dc-QPC (which is subject to 1∕f1∕f1∕f noise).