“…To address this concern, we generalize the physical idea of the so-called shortcuts to adiabaticity (STA) [34][35][36][37][38][39][40][41][42][43] method to accelerate the cooling process but keep the merits of the adiabatic passage. The STA method constructs an explicitly auxiliary Hamiltonian Ĥcd (t) to eliminate nonadiabatic transitions and compel the system to follow the eigenstates of Ĥapp (t) [38,39], thus implementing perfect excitation transfer at finite evolution periods [44][45][46]. In particular, the STA method has been experimentally implemented in various platforms [47][48][49][50][51][52][53][54][55][56][57][58][59][60], including nitrogen-vacancy-center systems [47,50,58], trapped ions [48,54], cold-atom systems [49,52], superconducting circuits [51,53,56,57,59], and nuclearmagnetic-resonance systems [55,60].…”