The delta function is a generalized function that can be defined as the limit of a class of delta sequences. The delta function is sometimes called "Dirac's delta function" or the "impulse symbol" (Bracewell 1999). It is implemented in the Wolfram Language as DiracDelta[x].
Formally, is a linear functional from a space (commonly taken as a Schwartz space or the space of all smooth functions of compact support ) of test functions . The action of on , commonly denoted or , then gives the value at 0 of for any function . In engineering contexts, the functional nature of the delta function is often suppressed.
The delta function can be viewed as the derivative of the Heaviside step function,
(1)

(Bracewell 1999, p. 94).
The delta function has the fundamental property that
(2)

and, in fact,
(3)

for .
Additional identities include
(4)

for , as well as
(5)
 
(6)

More generally, the delta function of a function of is given by
(7)

where the s are the roots of . For example, examine
(8)

Then , so and , giving
(9)

The fundamental equation that defines derivatives of the delta function is
(10)

Letting in this definition, it follows that
(11)
 
(12)
 
(13)

where the second term can be dropped since , so (13) implies
(14)

In general, the same procedure gives
(15)

but since any power of times integrates to 0, it follows that only the constant term contributes. Therefore, all terms multiplied by derivatives of vanish, leaving , so
(16)

which implies
(17)

Other identities involving the derivative of the delta function include
(18)

(19)

(20)

where denotes convolution,
(21)

and
(22)

An integral identity involving is given by
(23)

The delta function also obeys the socalled sifting property
(24)

(Bracewell 1999, pp. 7475).
A Fourier series expansion of gives
(25)
 
(26)
 
(27)
 
(28)

so
(29)
 
(30)

The delta function is given as a Fourier transform as
(31)

Similarly,
(32)

(Bracewell 1999, p. 95). More generally, the Fourier transform of the delta function is
(33)

The delta function can be defined as the following limits as ,
(34)
 
(35)
 
(36)
 
(37)
 
(38)
 
(39)
 
(40)

where is an Airy function, is a Bessel function of the first kind, and is a Laguerre polynomial of arbitrary positive integer order.
The delta function can also be defined by the limit as
(41)

Delta functions can also be defined in two dimensions, so that in twodimensional Cartesian coordinates
(42)

(43)

(44)

and
(45)

Similarly, in polar coordinates,
(46)

(Bracewell 1999, p. 85).
In threedimensional Cartesian coordinates
(47)

(48)

and
(49)

(50)

(51)

(Bracewell 1999, p. 85).
A series expansion in cylindrical coordinates gives
(52)
 
(53)

The solution to some ordinary differential equations can be given in terms of derivatives of (Kanwal 1998). For example, the differential equation
(54)

has classical solution
(55)

and distributional solution
(56)

(M. Trott, pers. comm., Jan. 19, 2006). Note that unlike classical solutions, a distributional solution to an thorder ODE need not contain independent constants.