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Briefly said: Every constant-coefficients [[Linear partial differential equation|linear partial differential equation]] on ${\bf R} ^ { n }$ can be solved.

Let $P$ be a [[Polynomial|polynomial]] in $n$ variables, $P ( \xi ) = \sum _ { J } a _ { J } \xi ^ { J }$, where the sum is a finite one, each $J$ is a multi-index $J = ( j _ { 1 } , \ldots , j _ { n } ) \in \mathbf{N} ^ { n }$, and $\xi ^ { J } = \xi _ { 1 } ^ { j_1 } \ldots \xi _ { n } ^ { j_n }$. To $P$ one associates a constant-coefficient linear partial differential operator $P ( D )$, obtained by replacing $\xi_j$ by $- i \partial / \partial x _ { j }$ ($i = \sqrt { - 1 }$).

Although several special cases had been known for a long time, it is only in the mid 1950s that it has been shown that for every non-zero constant-coefficient linear partial differential operator the equation $P ( D ) ( u ) = g$ can be solved for all functions or distributions (cf. also [[Generalized function|Generalized function]]) $g$ on ${\bf R} ^ { n }$. In particular, there is a distribution $E$ such that $P ( D ) ( E ) = \delta _ { 0 }$, where $\delta _ { 0 }$ is the Dirac mass at $0$ (cf. also [[Dirac delta-function|Dirac delta-function]]). Such an $E$ is called a fundamental solution. This is the celebrated Malgrange–Ehrenpreis theorem (established independently by B. Malgrange [[#References|[a8]]] and L. Ehrenpreis [[#References|[a1]]]). In case of the [[Laplace operator|Laplace operator]], the [[Newton potential|Newton potential]] (up to some factor) is a fundamental solution.

If $g$ is any distribution on ${\bf R} ^ { n }$ with compact support, by using a fundamental solution $E$ it is immediate to solve the equation $P ( D ) ( u ) = g$. Indeed ($*$ denoting convolution, cf. also [[Convolution of functions|Convolution of functions]]),

\begin{equation*} P ( D ) ( E *  g ) = ( P ( D ) ( E ) ) * g = \delta _ { 0 } * g = g. \end{equation*}

The Malgrange–Ehrenpreis theory goes further. One can solve the equation for non-compactly supported right-hand side $g$ by exhausting ${\bf R} ^ { n }$ by balls, and by solving the equation on each ball. The process is made to converge by corrections based on the approximation of local solutions to the homogeneous equation $P ( D ) u = 0$ by global solutions. The space of solutions to a linear homogeneous ordinary differential equation, with constant coefficients (for example, $y ^ { \prime \prime } + b y ^ { \prime } + c y = 0$), is spanned by exponential solutions $x \mapsto e ^ { r x }$ (in the example, $r$ is a root of $r ^ { 2 } + b r + c = 0$), or by exponential and possibly polynomial-exponential solutions ($x e ^ { rx }$ in the case of a double root). Similarly, the solutions to $P ( D ) u = 0$ can be approximated, on convex sets, by linear combinations of polynomial-exponential solutions, functions of the type $Q ( x ) e ^ { i \xi x }$, where $Q$ is a polynomial and necessarily $P ( \xi ) = 0$. See [[#References|[a2]]], [[#References|[a8]]], [[#References|[a5]]], (7.3.6). More generally, convolution equations can be considered.

Most often, the Malgrange–Ehrenpreis theorem is attacked by using the [[Fourier transform|Fourier transform]]. If $\phi$ is a $C ^ { \infty }$-function on ${\bf R} ^ { n }$, say with compact support, its Fourier transform is defined by

\begin{equation*} \hat { \phi } ( \xi ) = \int _ { \mathbf{R} ^ { n } } \phi ( x ) e ^ { - i \xi x } d x, \end{equation*}

and one has $( P ( D ) ( \phi ) )_{ \widehat{}} ( \xi ) = P ( \xi ) \widehat { \phi } ( \xi )$. Looking for a fundamental solution basically consists in solving the equation $\hat { E } = 1 / P ( \xi )$. This is of course totally elementary in case the function $1 / P ( \xi )$ is integrable on ${\bf R} ^ { n }$, since then, by inverse Fourier transformation, one can define (classically) $E$ by

\begin{equation*} E ( x ) = \frac { 1 } { ( 2 \pi ) ^ { n } } \int _ { \mathbf{R} ^ { n } } \frac { 1 } { P ( \xi ) } e ^ { i \xi x } d \xi . \end{equation*}

(For example, with $\Delta$ denoting the usual Laplacian, the operator $P ( D ) = I + ( - \Delta ) ^ { N }$, for $N &gt; n / 2$, for which $P ( \xi ) = 1 + | \xi | ^ { 2 N }$.)

In general, one has to face two problems: the lack of integrability at infinity of $1 / P ( \xi )$, and the real zeros of the polynomial $P$. Roughly speaking, since the two problems are not disjoint, one overcomes the first difficulty by the calculus of distributions, and the second one by switching to the complex domain. Both Malgrange and Ehrenpreis used the [[Hahn–Banach theorem|Hahn–Banach theorem]]. By now (1998) things have been much simplified, and a quick  "constructive"  proof of the Malgrange–Ehrenpreis theorem can be found in [[#References|[a5]]], (7.3.10), see also [[#References|[a3]]], (1.56). A formula claimed to be more explicit was recently given by H. König [[#References|[a7]]].

The solvability of constant-coefficients linear partial differential operators can also be studied with pure $L^{2}$ methods. There is a remarkable fundamental result by L.V. Hörmander [[#References|[a4]]], (2.6), whose proof is totally elementary, brief, and a masterpiece:

If $\Omega$ is a bounded set in ${\bf R} ^ { n }$, and if $P ( D )$ is non-zero, there exists a constant $C &gt; 0$ such that for every $C ^ { \infty }$-function $\phi$ with compact support in $\Omega$,

\begin{equation*} \| P ( D ) ( \phi ) \| _ { 2 } \geq C \| \phi \| _ { 2 } ( L ^ { 2 } \text { norms } ). \end{equation*}

It then follows, from elementary [[Hilbert space|Hilbert space]] theory, that the adjoint operator $P ^ { * } ( D )$ (associated to the polynomial $\overline { P ( - \xi ) }$) is solvable in $L ^ { 2 } ( \Omega )$. From there, one can recover the Malgrange–Ehrenpreis theorem. See [[#References|[a10]]], or [[#References|[a9]]] for an elementary exposition. However, the problem being not only to show the existence of a fundamental solution, but to get solutions with good properties, the construction in [[#References|[a5]]], Chap. 7, seems close to being optimal, see [[#References|[a6]]], Chap. 10.

The situation is radically different for operators with variable coefficients (see [[Lewy operator and Mizohata operator|Lewy operator and Mizohata operator]]).

====References====
<table><tr><td valign="top">[a1]</td> <td valign="top">  L. Ehrenpreis,   "Solutions of some problems of division I"  ''Amer. J. Math.'' , '''76'''  (1954)  pp. 883–903</td></tr><tr><td valign="top">[a2]</td> <td valign="top">  L. Ehrenpreis,   "Solutions of some problems of division II"  ''Amer. J. Math.'' , '''78'''  (1956)  pp. 685–715</td></tr><tr><td valign="top">[a3]</td> <td valign="top">  G.B. Folland,   "Introduction to partial differential equations" , Princeton Univ. Press  (1995)</td></tr><tr><td valign="top">[a4]</td> <td valign="top">  L. Hörmander,   "On the theory of general partial differential operators"  ''Acta Math.'' , '''94'''  (1955)  pp. 161–258</td></tr><tr><td valign="top">[a5]</td> <td valign="top">  L. Hörmander,   "The analysis of linear partial differential operators I" , ''Grundl. Math. Wissenschaft.'' , '''256''' , Springer  (1983)</td></tr><tr><td valign="top">[a6]</td> <td valign="top">  L. Hörmander,   "The analysis of linear partial differential operators II" , ''Grundl. Math. Wissenschaft.'' , '''257''' , Springer  (1983)</td></tr><tr><td valign="top">[a7]</td> <td valign="top">  H. König,   "An explicit formula for fundamental solutions of linear partial differential equations with constant coefficients"  ''Proc. Amer. Math. Soc.'' , '''120'''  (1994)  pp. 1315–1318</td></tr><tr><td valign="top">[a8]</td> <td valign="top">  B. Malgrange,   "Existence et approximation des solutions des équations aux dérivées partielles et des équations de convolution"  ''Ann. Inst. Fourier (Grenoble)'' , '''6'''  (1955/6)  pp. 271–355</td></tr><tr><td valign="top">[a9]</td> <td valign="top">  J-P. Rosay,   "A very elementary proof of the Malgrange–Ehrenpreis theorem"  ''Amer. Math. Monthly'' , '''98'''  (1991)  pp. 518–523</td></tr><tr><td valign="top">[a10]</td> <td valign="top">  F. Treves,   "Thèse d'Hörmander"  ''Sém. Bourbaki'' , '''Exp. 130'''  (1956)</td></tr></table>