“…Almost all classes of the DTQW except for a one-dimensional one with a two-dimensional coin [24,38,39] have the aspect of the localization defined that the limit distribution of the DTQW divided by some power of the time variable has the probability density given by the Dirac delta function. In the one dimensional DTQW, the localization was shown in the models with a three-dimensional coin [29], a four-dimensional coin [28], a two-dimensional coin with memory [56], a two-dimensional coin in a random environment [31], two-dimensional coins [48], an spatially incommensurate coin [70] and a time-dependent two-dimensional coin on the Fibonacci quantum walk [63] and a random coin [30,58]. On the other hand, the nature of the localization in the two-dimensional DTQW has been studied numerically [51,78] and analytically [27,81].…”