Fig. 3: Benchmarking of a Fsim gate with \(\theta=\frac{\pi }{4},\,\phi=\frac{\pi }{2}\). | Nature Communications

Fig. 3: Benchmarking of a Fsim gate with \(\theta=\frac{\pi }{4},\,\phi=\frac{\pi }{2}\).

From: Benchmarking universal quantum gates via channel spectrum

Fig. 3

In a, we fix the unitary error with δθ = −0.01, δϕ = −0.02, and vary the probability of stochastic error δp. In Fig. 3b, we fix the probability of stochastic error with δp = 0.001 and vary the angles of unitary error with δθ = 0.5δϕ = 10−3–10−1. We always accurately estimate the process infidelity and the stochastic infidelity of the gate. However, the accuracy of estimating the angles of the unitary error is compromised when there is a high level of stochastic noise, as the signal degrades quickly and there is not enough data to accurately estimate the angles.

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