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A method for solving linear differential equations for given boundary value or initial conditions, consisting in the transition from the given equation to an equation for an integral transform of the unknown function. The latter equation may turn out to be simpler. Suppose, e.g., that one has to find the solution to the equation

$$ \tag{1 }
a _ {0} ( x) 
\frac{d  ^ {2} u }{dx  ^ {2} }
 + a _ {1} ( x) 
\frac{du}{dx}

+ a _ {2} u  =  f ( x)
$$

on a finite or infinite interval with boundary conditions  $  u ( \alpha )= u _  \alpha  $, 
$  u ( \beta ) = u _  \beta  $. 
If the kernel  $  K ( s , x ) $
of the integral transformation

$$ 
\overline{u}\; ( s)  =  \int\limits _  \alpha  ^  \beta   K ( s , x ) u ( x)  dx
$$

satisfies the equation

$$ \tag{2 }

\frac{d  ^ {2} ( a _ {0} K  ) }{dx  ^ {2} }
 - 
\frac{d ( a _ {1} K  ) }{dx}
 + a _ {2} K  =  \lambda ( s) K ,
$$

where  $  \lambda ( s) $
is a function of  $  s $, 
then after multiplication of (1) by  $  K ( s , x ) $
and integration by parts over  $  ( \alpha , \beta ) $
one obtains the equation

$$ 
\left . \overline{f}\; ( s) -
\left [ a _ {0} \left ( K 
\frac{du}{dx}
 - u 
\frac{dK}{dx}
 \right ) +
\left ( a _ {1} - a _ {0}  ^  \prime  \right ) \right ]
\right | _ {x = \alpha }  ^ {x = \beta }  =  \lambda ( s) \overline{u}\; .
$$

Solving it for  $  \overline{u}\; ( s) $
and using an inversion formula for the integral transformation, one finds  $  u ( x) $. 
An analogous integral-transform method is used for partial differential equations.

Thus, the process for solving differential equations by this method consists of the following stages:

1) The choice of a suitable integral transformation.

2) Multiplication of the equation and boundary-initial conditions by the kernel of this integral transformation, and subsequent integration, over a suitable range, with respect to the independent variable  $  x $.

3) In the integration of 2), the use of the boundary-initial conditions to compute the terms arising from the integration limits.

4) Solution of the auxiliary equation and search for the integral transform of the unknown function.

5) Determination of the unknown function by an inversion formula.

====References====
<table><TR><TD valign="top">[1]</TD> <TD valign="top">  C.J. Tranter,   "Integral transformations in mathematical physics" , Wiley  (1966)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top">  R. Courant,   D. Hilbert,   "Methods of mathematical physics. Partial differential equations" , '''1–2''' , Interscience  (1953–1962)  (Translated from German)</TD></TR></table>

====Comments====
In many cases the interval of integration is infinite. Also, the path of integration is sometimes shifted into the complex plane.

Integral transformations which are widely used in this context are the [[Fourier transform|Fourier transform]] and the [[Laplace transform|Laplace transform]], cf., e.g., [[#References|[a1]]]–[[#References|[a3]]].

====References====
<table><TR><TD valign="top">[a1]</TD> <TD valign="top">  E.J. Watson,   "Laplace transforms and applications" , v. Nostrand-Reinhold  (1984)</TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top">  G. Doetsch,   "Introduction to the theory and application of the Laplace transformation" , Springer  (1974)  (Translated from German)</TD></TR><TR><TD valign="top">[a3]</TD> <TD valign="top">  R. Bracewell,   "The Fourier transform and its applications" , McGraw-Hill  (1965)</TD></TR></table>