“…Based on H I but with the redesigned Ω (1) d /2π = 250e −(t−τ d ) 2 /τ 2 MHz and Ω (1) m /2π = 250e −(t−τ m ) 2 /τ 2 MHz for t ∈ [0, 250 ns], we also have a full transfer from |e0 to |g1 in the adiabatic case, with τ d = 95 ns, τ = 50 ns, and τ m = 155 ns. However, due to noise effects existing in a process of longer duration time, the fidelity of adiabatic operation significantly degrades to be F A = 74.33% for the same decay rates, where F A has a definition same as that in equation (18). As an example illustration, we comparatively analyze the dependencies of F and F A on κ for the given γ and γ φ , see table 1.…”