Since the integral exists at each point, it can be differentiated inside the integral sign where it gives another compactly supported integrand, thus these functions are smooth (). What’s more, since the Paley–Wiener theorem holds, they are analytic.
To this space also belongs the function,
Definition 2 A function is a solution if:
i) for all ;
ii) its Fourier transform, , is continuous, and vanishes for where is some constant independent of ;
iii) is a classical solution; that is exists and satisfies the equation at each point .
a direct application of the uniqueness of the Fourier representation for smooth functions shows:
Lemma 1 Given a constant coefficients linear evolution equation, for each initial data in there exists a unique solution and it is given by the above formula.
Thus we see that there are plenty of smooth solutions, whatever the system is. But it was realized by Hadamard  that there were not enough solutions, since the space is not closed. Furthermore, in general there are no topologies on the space of initial data, and of solutions for which solutions depend continuously on initial data. Lack of continuity of solutions with respect to their initial data would not only imply lack of predictability from the physical standpoint, for all data are subject to measurement errors, but also lack of realistic possibilities of numerically computing solutions, due to truncation errors. Thus it is important to characterize the set of equations for which continuity holds. There are several possibilities for the choice of the topologies for the spaces of initial data and of solutions. Here we restrict consideration to those which have been more prolific with respect to results and generalizations to non-linear, non-constant coefficient equations systems.
Definition 3 A system of partial differential equations is called well posed if there exists a norm (usually a Sobolev norm) and two constants, , , such that for all initial data in and all positive times,
Theorem 1 A system is well posed if and only if there exists constants and such that for all positive times,
where the above norm is the usual operator norm on matrices.
If a system is well posed for the norm, [recall that the norm of a function is the square root of the integral of its square], then it is well posed for any other Sobolev norm, (as follows from the above theorem), since the constants are independent of . The above theorem reduces the problem of well posedness to an algebraic one which we further refine in the following theorem:
Theorem 2 [Kreiss  The following conditions are equivalent:
i) The system is well posed.
ii) There exist constants , and , and a positive definite Hermitian form such that:
This result is central to the theory. The proof that ii) implies i) is simple and follows directly from the inequality:
© Max Planck Society and the author(s)