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arXiv 1111.7272cond-mat.supr-concond-mat.mes-hallquant-ph
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谱密度标度为$1/ f^α$的通量噪声引起的通量量子比特的纯退相

Pure dephasing in flux qubits due to flux noise with spectral density scaling as $1/ f^α$

S. M. Anton, C. Müller, J. S. Birenbaum, S. R. O'Kelley, A. D. Fefferman, D. S. Golubev, G. C. Hilton, H. -M. Cho, K. D. Irwin, F. C. Wellstood, Gerd Schön, A. … 展开作者

S. M. Anton, C. Müller, J. S. Birenbaum, S. R. O'Kelley, A. D. Fefferman, D. S. Golubev, G. C. Hilton, H. -M. Cho, K. D. Irwin, F. C. Wellstood, Gerd Schön, A. Shnirman, John Clarke

摘要:

对于许多类型的超导量子比特,磁通噪声是纯退相的来源。在一个具有代表性的直流超导量子干涉仪(SQUID)上,在一定温度范围内的测量结果表明,$S_Φ(f) = A^2/(f/1 \hbox{Hz})^α$,其中$S_Φ$是磁通噪声谱密度,$A$是1 $μΦ_0 \, \hbox{Hz}^{-1/2}$和$0.61 \leq α\leq 0.95$的数量级; $Φ_{0}$是磁通量子。对于能级分裂线性耦合到所施加的通量的量子比特,计算的纯退相时间$τ_ϕ$的拉姆齐和回波脉冲序列的$τ_ϕ$的$α$固定$A$的依赖性表明,$τ_ϕ$迅速减少$α$减少。我们发现,$τ_ϕ$是相对不敏感的噪声带宽,$f_1 \leq f \leq f_2$,所有的$α$提供的紫外截止频率$f_2 > 1/τ_ϕ$。我们计算了回波序列($E$)和拉姆齐序列($R$)的比值$τ_{ϕ,E} / τ_{ϕ,R}$,以及衰减函数对$α$和$f_2$的依赖性。我们调查的情况下,其中$S_Φ(f_0)$是固定的“枢轴频率”$f_0 \neq 1$ Hz,而$α$是变化的,并发现$f_0$的选择可以极大地影响的灵敏度$τ_{ϕ,E}$和$τ_{ϕ,R}$的$α$值。最后,我们提出了计算值的$τ_ϕ$在一个量子位对应的值的$A$和$α$在我们的SQUID测量。

英文摘要:

For many types of superconducting qubits, magnetic flux noise is a source of pure dephasing. Measurements on a representative dc superconducting quantum interference device (SQUID) over a range of temperatures show that $S_Φ(f) = A^2/(f/1 \hbox{Hz})^α$, where $S_Φ$ is the flux noise spectral density, $A$ is of the order of 1 $μΦ_0 \, \hbox{Hz}^{-1/2}$ and $0.61 \leq α\leq 0.95$; $Φ_{0}$ is the flux quantum. For a qubit with an energy level splitting linearly coupled to the applied flux, calculations of the dependence of the pure dephasing time $τ_ϕ$ of Ramsey and echo pulse sequences on $α$ for fixed $A$ show that $τ_ϕ$ decreases rapidly as $α$ is reduced. We find that $τ_ϕ$ is relatively insensitive to the noise bandwidth, $f_1 \leq f \leq f_2$, for all $α$ provided the ultraviolet cutoff frequency $f_2 > 1/τ_ϕ$. We calculate the ratio $τ_{ϕ,E} / τ_{ϕ,R}$ of the echo ($E$) and Ramsey ($R$) sequences, and the dependence of the decay function on $α$ and $f_2$. We investigate the case in which $S_Φ(f_0)$ is fixed at the "pivot frequency" $f_0 \neq 1$ Hz while $α$ is varied, and find that the choice of $f_0$ can greatly influence the sensitivity of $τ_{ϕ,E}$ and $τ_{ϕ,R}$ to the value of $α$. Finally, we present calculated values of $τ_ϕ$ in a qubit corresponding to the values of $A$ and $α$ measured in our SQUID.

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