“…When we reformulate the above equations in the Gevrey distributions we do not follow the method using operators in [2], [3], [4] and [10], [11], but use fundamental properties of generalized functions such as the tensor product and the pullback of Gevrey distributions. In fact, this method gives essentially the same formulation as in [2], [3], [4] and [10], [11], but the final form of each equation looks like the classical one.…”