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arXiv 0908.3937cond-mat.supr-con
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基于强非简谐约瑟夫森振子的超导相位量子比特

Superconducting phase qubit based on the Josephson oscillator with strong anharmonicity

A. B. Zorin, F. Chiarello

摘要:

在屏蔽参数为$β_L = (2π/Φ_0)LI_c \approx 1$的射频SQUID的基础上,提出了一种超导相位量子比特,并由半通量量子$Φ_e=Φ_0/2$偏置。由于余弦约瑟夫森势和抛物线磁能势的相互作用,可以在该系统中实现显著的非谐性($> 30%$),该非谐性最终导致阱的四次多项式形状。这个全局最小值中的两个最低本征态完全适合于对电荷变量不敏感的量子位,偏置在最佳点,并允许有效的色散读出。此外,该量子位中的跃迁频率可以在允许可变量子位-量子位耦合的可观范围内调谐。

英文摘要:

We propose a superconducting phase qubit on the basis of the radio-frequency SQUID with the screening parameter value $β_L = (2π/Φ_0)LI_c \approx 1$, biased by a half flux quantum $Φ_e=Φ_0/2$. Significant anharmonicity ($> 30%$) can be achieved in this system due to the interplay of the cosine Josephson potential and the parabolic magnetic-energy potential that ultimately leads to the quartic polynomial shape of the well. The two lowest eigenstates in this global minimum perfectly suit for the qubit which is insensitive to the charge variable, biased in the optimal point and allows an efficient dispersive readout. Moreover, the transition frequency in this qubit can be tuned within an appreciable range allowing variable qubit-qubit coupling.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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