“…Compared to the two-state scenario, the research of generalized Landau-Zener transition for complicated systems with more than two states, even in ordinary Hermitian quantum mechanics, has been arduous and in most cases inconclusive. The main reason is that in conventional Landau-Zener transition, the coupling equations which govern the non-adiabatic transition amplitudes between the two energy levels can be reduced to a single second-order differential equation, e.g., the parabolic cylinder function for linear separation of diabatic energies [16], or the confluent Heun functions for quadratic and cubic separations of diabatic energies [23,24]. In contrast, in the general multi-state scenario, if one attempts to re-duce the coupling equations which govern the non-adiabatic transition amplitudes between different energy levels in a single equation, one would probably obtain an ordinary differential equation with order greater than two.…”