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高保真度双量子比特门对实现容错量子计算至关重要, 是量子计算领域重点研究内容之一. 量子门的保真度会受到量子芯片参数、控制波形等多种因素影响. 本文系统地研究了芯片参数、控制波形、耦合器起始频率、比特频率等对CZ门保真度的影响, 在此基础上进一步研究了门保真度对控制参数偏离的响应. 在芯片设计方案层面, 基于CBQ参数的量子芯片可以在更短的门操作时间实现更高保真度的CZ门. 控制波形方面, 三级傅里叶级数波相较方波和圆角梯形波在门错误率和门操作时间两方面均更为出色, 更能满足高效实现高保真度量子门的要求. 耦合器起始频率以及量子比特频率等因素对CZ门保真度的影响则相对较小, 在很宽的频率范围内, 总是可以通过优化控制波形参数实现高保真度的CZ门; 而轻微的控制参数偏离则会导致门错误率显著上升. 本研究对于厘清各因素对CZ门保真度的影响具有重要意义, 可为超导量子芯片设计及高保真度CZ门实验实现提供理论与技术支撑, 助力量子计算工程化发展.Efficient and high-fidelity two-qubit gates are crucial to achieving fault-tolerant quantum computing and have become one of the key research topics in the quantum computing field. The fidelity of quantum gates is affected by many factors, such as quantum chip parameters and control waveforms. In theory, the chip paramters and waveforms can be precisely designed. However, in practice, the actual chip parameters and waveforms may deviate from the theoretical values. It is necessary to systematically study the effects of chip parameters, control waveforms, and other factors on the fidelity of two-qubit gates, and determine the magnitude and direction of the each factor's effect. Here, we systematically study the effects of chip parameters, control waveforms, coupler start frequency, qubit frequency, etc. on the fidelity of CZ gates. On this basis, the response of gate fidelity to deviations in control parameters is further studied. At the chip design level, quantum chips based on CBQ parameters can achieve higher-fidelity CZ gates in shorter gate operation time. In terms of controlling waveforms, the three-level Fourier series wave is superior to the square wave and rounded trapezoidal wave in achieving lower gate error rate and shorter gate operation time, and can better meet the requirements for efficient implementation of high-fidelity quantum gates. Factors such as the coupler starting frequency and qubit frequency have relatively little effect on the fidelity of the CZ gate. In a wide frequency range, high-fidelity CZ gates can always be achieved by optimizing the control waveform parameters. It should be pointed out that slight deviations of control parameters will lead to a significant increase in the gating error. This study is of great significance for clarifying the effects of various factors on the fidelity of the CZ gate. It can provide theoretical and technical support for designing superconducting quantum chips and realizing high-fidelity CZ gate, thereby promoting the engineering development of quantum computing.
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Keywords:
- quantum computing /
- quantum gates /
- quantum control /
- fidelity
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图 1 三种不同$ \omega_{{\mathrm{c}}}(t) $波形示意图. 图(a)和(b)是方波, (c)和(d)是圆角梯形波, (e)和(f)是傅里叶级数波. 图(a)、(c)和(e)对应着$ \omega_{{\mathrm{c}}}^{{\rm{off}}} $ < $ \omega_{{\mathrm{c}}}^{{\rm{on}}} $的情形, 而图(b)、(d)和(f)对应着$ \omega_{{\mathrm{c}}}^{{\rm{off}}} $ > $ \omega_{{\mathrm{c}}}^{{\rm{on}}} $的情形. 图(e)和(f)中的三条细虚线对应着傅里叶级数波形的三个分量: $ \omega_{{\mathrm{c}}}^{{\rm{off}}} + \lambda_{m} \left( 1 - \cos \dfrac{2 \pi m t}{t_{{\mathrm{gate}}}} \right), m=1, 2, 3 $
Fig. 1. Schematic diagram of square pulse ((a) and (b)), rounded-trapezoid-shaped pulse ((c) and (d)) and Fourier-series pulse ((e) and (f)). (a), (c), and (e) correspond to the case where $ \omega_{{\mathrm{c}}}^{{\rm{off}}} $ < $ \omega_{{\mathrm{c}}}^{{\rm{on}}} $, and (b), (d), and (f) correspond to the case where $ \omega_{{\mathrm{c}}}^{{\rm{off}}} $ > $ \omega_{{\mathrm{c}}}^{{\rm{on}}} $. The three thin dashed lines in (e) and (f) correspond to the three components of the Fourier series pulse: $ \omega_{{\mathrm{c}}}^{{\rm{off}}} + \lambda_{m} \left( 1 - \cos \dfrac{2 \pi m t}{t_{{\mathrm{gate}}}} \right), m=1, 2, 3 $.
图 2 哈密顿量H和$ H_{0} $的能谱((a)和(c))以及ZZ相互作用$ \left\lvert \zeta \right\rvert /2 \pi $((b)和(d))与耦合器频率$ \omega_{{\mathrm{c}}}/2\pi $的关系. (a)和(b)对应CAQ模型参数; (c)和(d)对应CBQ模型参数; 图(a)和(c)中的黑色虚线对应着无相互作用哈密顿量$ H_{0} $的本征能量, 彩色实线对应着系统哈密顿量H的本征能量
Fig. 2. Energy-level spectra ((a) and (c)) and ZZ interaction $ \left\lvert \zeta \right\rvert /2 \pi $ ((b) and (d)) of the system Hamiltonian H as a function of the coupler frequency $ \omega_{{\mathrm{c}}}/2\pi $. Figure (a) and (b) correspond to the CAQ model parameters, and figure (c) and (d) correspond to the CBQ model parameters. The black dashed lines in figure (a) and (c) corresponds to the eigen-energies of the non-interacting Hamiltonian $ H_{0} $, and the colored solid lines correspond to the eigen-energies of the system Hamiltonian H.
图 3 不同模型参数下的CZ门错误率. 图(a)和图(b)分别对应CAQ和CBQ两组模型参数. 图中蓝色、绿色和红色实线分别对应$ m_{\max} = 1, 2, 3 $三种不同的傅里叶级数波形
Fig. 3. CZ gate errors under different model parameters. Figure (a) and (b) correspond to the CAQ and CBQ model parameters, respectively. The blue, green, and red solid lines in the figures correspond to three different Fourier series pulses with $ m_{\max} $ = 1, 2, and 3, respectively.
图 4 (a) 方波对应的CZ门错误率; (b) 圆角梯形波对应的CZ门错误率; 傅里叶级数波对应的CZ门错误率见图3(b). (a)、(b)和图3(b)均是采用CBQ模型参数计算所得
Fig. 4. (a) CZ gate errors under square pulse; (b) CZ gate errors under rounded-trapezoid-shaped pulse; for CZ gate errors under Fourier-series pulse, see Fig. 3(b). Both (a), (b) and Fig. 3(b) are calculated using CBQ model parameters.
图 5 不同$ \omega_{c}^{{\rm{off}}} $下的CZ门错误率. 每一行的五张子图((a1)—(e1)以及(a2)—(e2))对应的$ \omega_{{\mathrm{c}}}^{{\rm{off}}} $分别为3594、3636、3678、3800和4000 MHz, 其他参数同CBQ模型参数. (a1)—(e1)的门错误率是使用$ H_{0} $的本征态计算的, 见公式(11); (a2)—(e2)的门错误率是使用系统哈密顿量H的本征态计算的, 见公式(12). (f)和(g)是采用傅里叶级数波形时的门错误率, 分别对应$ \omega_{{\mathrm{c}}}^{{\rm{off}}} = 3594, $$ 3678 $ MHz
Fig. 5. CZ gate errors rate under different $ \omega_{{\mathrm{c}}}^{{\rm{off}}} $. The corresponding $ \omega_{{\mathrm{c}}}^{{\rm{off}}} $ of the five sub-figures ((a1)–(e1) and (a2)–(e2)) in each row are: 3594, 3636, 3678, 3800 and 4000 MHz respectively, other model paramters are the same as CBQ. The gate errors in (a1)–(e1) are calculated using the eigenstates of $ H_{0} $, see Eq(11); (a2)–(e2) are calculated using the eigenstates of H, see Eq(12). (f) and (g) are the gate error rates with Fourier series pulse, $ \omega_{{\mathrm{c}}}^{{\rm{off}}} = 3594, 3678 $ MHz, respectively.
图 6 不同量子比特频率$ \omega_{2} $下的CZ门错误率, 横轴是门操作时间$ t_{{\mathrm{gate}}} $, 纵轴是量子比特$ Q_{2} $的比特频率$ \omega_{2} $, 一共选取了$ \omega_{2} / 2 \pi = 4.0, 4.1, 4.2, 4.3, 4.4, 4.5, 4.6, 4.7, 4.8, 4.9, $$ 4.95 $ GHz共11个不同的$ \omega_{2} $值, 其他模型参数同CBQ模型参数. (a)—(c)分别对应傅里叶分量数目$ m_{\max} = 1, 2, 3 $的情形
Fig. 6. CZ gate error under different qubit frequencies $ \omega_{2} $. The horizontal axis is the gate operation time $ t_{{\mathrm{gate}}} $, and the vertical axis is the qubit frequency $ \omega_{2} $ of the $ Q_{2} $. A total of 11 different $ \omega_{2} $ values were selected, including $ \omega_{2} / 2 \pi = $$ 4.0, 4.1, 4.2, 4.3, 4.4, 4.5, 4.6, 4.7, 4.8, 4.9, 4.95 $ GHz. Other model parameters are the same as the CBQ model parameters.
图 7 控制波形参数偏移对CZ门保真度的影响
Fig. 7. Effect of control waveform parameter deviation on CZ gate fidelity.
表 1 本文选取的两组模型参数, 分别标记为CAQ和CBQ
Table 1. The two sets of model parameters used in this paper, marked as CAQ and CBQ respectively.
模型参数 CAQ CBQ $ \rho_{1 {\mathrm{c}}} $ 0.0180 0.0220 $ \rho_{2 {\mathrm{c}}} $ 0.0180 –0.0220 $ \rho_{12} $ 0.0015 0.0013 $ \omega_{1} / 2 \pi \quad ({\rm{GHz}}) $ 6.0 5.0 $ \omega_{2} / 2 \pi \quad ({\rm{GHz}}) $ 5.4 4.8 $ \alpha_{1} / 2 \pi \quad ({\rm{MHz}}) $ –250.0 –220.0 $ \alpha_{2} / 2 \pi \quad ({\rm{MHz}}) $ –250.0 –220.0 $ \alpha_{c} / 2 \pi \quad ({\rm{MHz}}) $ –300.0 –170.0 
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表 2 不同$ \omega_{{\mathrm{c}}}^{{\rm{off}}} $下的CZ门错误率
Table 2. CZ gate errors rate under different $ \omega_{{\mathrm{c}}}^{{\rm{off}}} $.
$ \omega_{{\mathrm{c}}}^{{\rm{off}}} $ (MHz) Bare Dressed $ t_{{\mathrm{gate}}} (ns) $ $ \omega_{{\mathrm{c}}}^{{\rm{on}}} $ (MHz) $ E_{{\mathrm{g}}} $ $ t_{{\mathrm{gate}}} (ns) $ $ \omega_{{\mathrm{c}}}^{{\rm{on}}} $ (MHz) $ E_{{\mathrm{g}}} $ 3594 53/2.4 4514.0 7.2431e–3 43/2.4 4615.5 5.9816e–4 104/2.4 4582.5 9.1781e–3 93/2.4 4623.5 1.6110e–3 220/2.4 4144.0 5.5215e–3 212/2.4 4159.0 2.4819e–4 272/2.4 4327.5 5.1956e–3 273/2.4 4326.0 8.4726e–5 3636 54/2.4 4505.0 7.4825e–3 43/2.4 4614.5 5.0617e–4 114/2.4 4548.5 9.7407e–3 93/2.4 4623.5 1.4097e–4 220/2.4 4141.5 6.0894e–3 212/2.4 4158.5 2.3052e–4 272/2.4 4325.5 6.0173e–3 273/2.4 4326.0 7.3497e–5 3678 43/2.4 4612.5 7.3516e–3 43/2.4 4613.5 4.4968e–4 102/2.4 4587.5 6.6712e–3 93/2.4 4623.5 1.2503e–3 209/2.4 4163.0 6.3633e–3 213/2.4 4156.5 2.1617e–4 273/2.4 4325.5 6.2150e–3 273/2.4 4326.0 8.0159e–5 3800 41/2.4 4624.0 8.2440e–3 43/2.4 4610.5 4.9159e–4 101/2.4 4590.0 8.6945e–3 93/2.4 4622.0 1.0150e–3 209/2.4 4154.0 7.6224e–3 213/2.4 4155.5 1.7852e–4 271/2.4 4323.5 7.8218e–3 273/2.4 4325.5 1.0117e–5 4000 40/2.4 4610.0 1.0993e–2 53/2.4 4508.0 5.3763e–4 100/2.4 4584.5 6.1489e–3 105/2.4 4576.0 9.3363e–4 208/2.4 4148.0 1.1798e–2 218/2.4 4144.5 2.4616e–5 273/2.4 4318.0 1.1304e–2 274/2.4 4322.5 3.1172e–4
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