Dirac delta function
Differential equations 

Classification 
Solution 
In mathematical analysis, the Dirac delta function (or δ distribution), also known as the unit impulse,^{[1]} is a generalized function on the real numbers, whose value is zero everywhere except at zero, and whose integral over the entire real line is equal to one.^{[2]}^{[3]}^{[4]} Since there is no function having this property, to model the delta "function" rigorously involves the use of limits or, as is common in mathematics, measure theory and the theory of distributions.
The delta function was introduced by physicist Paul Dirac, and has since been applied routinely in physics and engineering to model point masses and instantaneous impulses. It is called the delta function because it is a continuous analogue of the Kronecker delta function, which is usually defined on a discrete domain and takes values 0 and 1. The mathematical rigor of the delta function was disputed until Laurent Schwartz developed the theory of distributions, where it is defined as a linear form acting on functions.
Motivation and overview
The graph of the Dirac delta is usually thought of as following the whole xaxis and the positive yaxis.^{[5]}^{:174} The Dirac delta is used to model a tall narrow spike function (an impulse), and other similar abstractions such as a point charge, point mass or electron point. For example, to calculate the dynamics of a billiard ball being struck, one can approximate the force of the impact by a Dirac delta. In doing so, one not only simplifies the equations, but one also is able to calculate the motion of the ball, by only considering the total impulse of the collision, without a detailed model of all of the elastic energy transfer at subatomic levels (for instance).
To be specific, suppose that a billiard ball is at rest. At time [math]\displaystyle{ t=0 }[/math] it is struck by another ball, imparting it with a momentum P, with units kg⋅m⋅s^{−1}. The exchange of momentum is not actually instantaneous, being mediated by elastic processes at the molecular and subatomic level, but for practical purposes it is convenient to consider that energy transfer as effectively instantaneous. The force therefore is P δ(t); the units of δ(t) are s^{−1}.
To model this situation more rigorously, suppose that the force instead is uniformly distributed over a small time interval [math]\displaystyle{ \Delta t = [0,T] }[/math]. That is,
[math]\displaystyle{ F_{\Delta t}(t) = \begin{cases} P/\Delta t& 0\lt t\leq T, \\ 0 &\text{otherwise}. \end{cases} }[/math]
Then the momentum at any time t is found by integration:
[math]\displaystyle{ p(t) = \int_0^t F_{\Delta t}(\tau)\,d\tau = \begin{cases} P & t \ge T\\ P\,t/\Delta t & 0 \le t \le T\\ 0&\text{otherwise.}\end{cases} }[/math]
Now, the model situation of an instantaneous transfer of momentum requires taking the limit as Δt → 0, giving a result everywhere except at 0:
[math]\displaystyle{ p(t)=\begin{cases}P & t \gt 0\\ 0 & t \lt 0.\end{cases} }[/math]
Here the functions [math]\displaystyle{ F_{\Delta t} }[/math] are thought of as useful approximations to the idea of instantaneous transfer of momentum.
The delta function allows us to construct an idealized limit of these approximations. Unfortunately, the actual limit of the functions (in the sense of pointwise convergence) [math]\displaystyle{ \lim_{\Delta t\to 0^+}F_{\Delta t} }[/math] is zero everywhere but a single point, where it is infinite. To make proper sense of the Dirac delta, we should instead insist that the property
[math]\displaystyle{ \int_{\infty}^\infty F_{\Delta t}(t)\,dt = P, }[/math]
which holds for all [math]\displaystyle{ \Delta t\gt 0 }[/math], should continue to hold in the limit. So, in the equation [math]\displaystyle{ F(t)=P\,\delta(t)=\lim_{\Delta t\to 0}F_{\Delta t}(t) }[/math], it is understood that the limit is always taken outside the integral.
In applied mathematics, as we have done here, the delta function is often manipulated as a kind of limit (a weak limit) of a sequence of functions, each member of which has a tall spike at the origin: for example, a sequence of Gaussian distributions centered at the origin with variance tending to zero.
The Dirac delta is not truly a function, at least not a usual one with domain and range in real numbers. For example, the objects f(x) = δ(x) and g(x) = 0 are equal everywhere except at x = 0 yet have integrals that are different. According to Lebesgue integration theory, if f and g are functions such that f = g almost everywhere, then f is integrable if and only if g is integrable and the integrals of f and g are identical. A rigorous approach to regarding the Dirac delta function as a mathematical object in its own right requires measure theory or the theory of distributions.
History
Joseph Fourier presented what is now called the Fourier integral theorem in his treatise Théorie analytique de la chaleur in the form:^{[6]}
[math]\displaystyle{ f(x)=\frac{1}{2\pi}\int_{\infty}^\infty\ \ d\alpha \, f(\alpha) \ \int_{\infty}^\infty dp\ \cos (pxp\alpha)\ , }[/math]
which is tantamount to the introduction of the δfunction in the form:^{[7]}
[math]\displaystyle{ \delta(x\alpha)=\frac{1}{2\pi} \int_{\infty}^\infty dp\ \cos (pxp\alpha) \ . }[/math]
Later, Augustin Cauchy expressed the theorem using exponentials:^{[8]}^{[9]}
[math]\displaystyle{ f(x)=\frac{1}{2\pi} \int_{\infty} ^ \infty \ e^{ipx}\left(\int_{\infty}^\infty e^{ip\alpha }f(\alpha)\,d \alpha \right) \,dp. }[/math]
Cauchy pointed out that in some circumstances the order of integration is significant in this result (contrast Fubini's theorem).^{[10]}^{[11]}
As justified using the theory of distributions, the Cauchy equation can be rearranged to resemble Fourier's original formulation and expose the δfunction as
[math]\displaystyle{ \begin{align} f(x)&=\frac{1}{2\pi} \int_{\infty}^\infty e^{ipx}\left(\int_{\infty}^\infty e^{ip\alpha }f(\alpha)\,d \alpha \right) \,dp \\[4pt] &=\frac{1}{2\pi} \int_{\infty}^\infty \left(\int_{\infty}^\infty e^{ipx} e^{ip\alpha } \,dp \right)f(\alpha)\,d \alpha =\int_{\infty}^\infty \delta (x\alpha) f(\alpha) \,d \alpha, \end{align} }[/math]
where the δfunction is expressed as
[math]\displaystyle{ \delta(x\alpha)=\frac{1}{2\pi} \int_{\infty}^\infty e^{ip(x\alpha)}\,dp \ . }[/math]
A rigorous interpretation of the exponential form and the various limitations upon the function f necessary for its application extended over several centuries. The problems with a classical interpretation are explained as follows:^{[12]}
 The greatest drawback of the classical Fourier transformation is a rather narrow class of functions (originals) for which it can be effectively computed. Namely, it is necessary that these functions decrease sufficiently rapidly to zero (in the neighborhood of infinity) to ensure the existence of the Fourier integral. For example, the Fourier transform of such simple functions as polynomials does not exist in the classical sense. The extension of the classical Fourier transformation to distributions considerably enlarged the class of functions that could be transformed and this removed many obstacles.
Further developments included generalization of the Fourier integral, "beginning with Plancherel's pathbreaking L^{2}theory (1910), continuing with Wiener's and Bochner's works (around 1930) and culminating with the amalgamation into L. Schwartz's theory of distributions (1945) ...",^{[13]} and leading to the formal development of the Dirac delta function.
An infinitesimal formula for an infinitely tall, unit impulse delta function (infinitesimal version of Cauchy distribution) explicitly appears in an 1827 text of Augustin Louis Cauchy. ^{[14]} Siméon Denis Poisson considered the issue in connection with the study of wave propagation as did Gustav Kirchhoff somewhat later. Kirchhoff and Hermann von Helmholtz also introduced the unit impulse as a limit of Gaussians, which also corresponded to Lord Kelvin's notion of a point heat source. At the end of the 19th century, Oliver Heaviside used formal Fourier series to manipulate the unit impulse.^{[15]} The Dirac delta function as such was introduced by Paul Dirac in his 1927 paper The Physical Interpretation of the Quantum Dynamics^{[16]} and used in his textbook The Principles of Quantum Mechanics.^{[3]} He called it the "delta function" since he used it as a continuous analogue of the discrete Kronecker delta.
Definitions
The Dirac delta function [math]\displaystyle{ \delta (x) }[/math] can be loosely thought of as a function on the real line which is zero everywhere except at the origin, where it is infinite,
[math]\displaystyle{ \delta(x) \simeq \begin{cases} +\infty, & x = 0 \\ 0, & x \ne 0 \end{cases} }[/math]
and which is also constrained to satisfy the identity^{[17]}
[math]\displaystyle{ \int_{\infty}^\infty \delta(x) \, dx = 1. }[/math]
This is merely a heuristic characterization. The Dirac delta is not a function in the traditional sense as no function defined on the real numbers has these properties.^{[18]}
As a measure
One way to rigorously capture the notion of the Dirac delta function is to define a measure, called Dirac measure, which accepts a subset A of the real line R as an argument, and returns δ(A) = 1 if 0 ∈ A, and δ(A) = 0 otherwise.^{[19]} If the delta function is conceptualized as modeling an idealized point mass at 0, then δ(A) represents the mass contained in the set A. One may then define the integral against δ as the integral of a function against this mass distribution. Formally, the Lebesgue integral provides the necessary analytic device. The Lebesgue integral with respect to the measure δ satisfies
[math]\displaystyle{ \int_{\infty}^\infty f(x) \, \delta(dx) = f(0) }[/math]
for all continuous compactly supported functions f. The measure δ is not absolutely continuous with respect to the Lebesgue measure—in fact, it is a singular measure. Consequently, the delta measure has no Radon–Nikodym derivative (with respect to Lebesgue measure)—no true function for which the property
[math]\displaystyle{ \int_{\infty}^\infty f(x)\, \delta(x)\, dx = f(0) }[/math]
holds.^{[20]} As a result, the latter notation is a convenient abuse of notation, and not a standard (Riemann or Lebesgue) integral.
As a probability measure on R, the delta measure is characterized by its cumulative distribution function, which is the unit step function.^{[21]}
[math]\displaystyle{ H(x) = \begin{cases} 1 & \text{if } x\ge 0\\ 0 & \text{if } x \lt 0. \end{cases} }[/math]
This means that H(x) is the integral of the cumulative indicator function 1_{(−∞, x]} with respect to the measure δ; to wit,
[math]\displaystyle{ H(x) = \int_{\mathbf{R}}\mathbf{1}_{(\infty,x]}(t)\,\delta(dt) = \delta(\infty,x], }[/math]
the latter being the measure of this interval; more formally, δ((−∞, x]). Thus in particular the integration of the delta function against a continuous function can be properly understood as a Riemann–Stieltjes integral:^{[22]}
[math]\displaystyle{ \int_{\infty}^\infty f(x)\,\delta(dx) = \int_{\infty}^\infty f(x) \,dH(x). }[/math]
All higher moments of δ are zero. In particular, characteristic function and moment generating function are both equal to one.
As a distribution
In the theory of distributions, a generalized function is considered not a function in itself but only through how it affects other functions when "integrated" against them.^{[23]} In keeping with this philosophy, to define the delta function properly, it is enough to say what the "integral" of the delta function is against a sufficiently "good" test function φ. Test functions are also known as bump functions. If the delta function is already understood as a measure, then the Lebesgue integral of a test function against that measure supplies the necessary integral.
A typical space of test functions consists of all smooth functions on R with compact support that have as many derivatives as required. As a distribution, the Dirac delta is a linear functional on the space of test functions and is defined by^{[24]}

[math]\displaystyle{ \delta[\varphi] = \varphi(0) }[/math]
(
)
for every test function φ.
For δ to be properly a distribution, it must be continuous in a suitable topology on the space of test functions. In general, for a linear functional S on the space of test functions to define a distribution, it is necessary and sufficient that, for every positive integer N there is an integer M_{N} and a constant C_{N} such that for every test function φ, one has the inequality^{[25]}
[math]\displaystyle{ \leftS[\varphi]\right \le C_N \sum_{k=0}^{M_N}\sup_{x\in [N,N]} \left\varphi^{(k)}(x)\right }[/math]
where sup represents the supremum. With the δ distribution, one has such an inequality (with C_{N} = 1) with M_{N} = 0 for all N. Thus δ is a distribution of order zero. It is, furthermore, a distribution with compact support (the support being Template:Brace).
The delta distribution can also be defined in several equivalent ways. For instance, it is the distributional derivative of the Heaviside step function. This means that for every test function φ, one has
[math]\displaystyle{ \delta[\varphi] = \int_{\infty}^\infty \varphi'(x)\,H(x)\,dx. }[/math]
Intuitively, if integration by parts were permitted, then the latter integral should simplify to
[math]\displaystyle{ \int_{\infty}^\infty \varphi(x)\,H'(x)\,dx = \int_{\infty}^\infty \varphi(x)\,\delta(x)\,dx, }[/math]
and indeed, a form of integration by parts is permitted for the Stieltjes integral, and in that case, one does have
[math]\displaystyle{ \int_{\infty}^\infty \varphi'(x)\,H(x)\, dx = \int_{\infty}^\infty \varphi(x)\,dH(x). }[/math]
In the context of measure theory, the Dirac measure gives rise to distribution by integration. Conversely, equation (1) defines a Daniell integral on the space of all compactly supported continuous functions φ which, by the Riesz representation theorem, can be represented as the Lebesgue integral of φ with respect to some Radon measure.
Generally, when the term Dirac delta function is used, it is in the sense of distributions rather than measures, the Dirac measure being among several terms for the corresponding notion in measure theory. Some sources may also use the term Dirac delta distribution.
Generalizations
The delta function can be defined in ndimensional Euclidean space R^{n} as the measure such that
[math]\displaystyle{ \int_{\mathbf{R}^n} f(\mathbf{x})\,\delta(d\mathbf{x}) = f(\mathbf{0}) }[/math]
for every compactly supported continuous function f. As a measure, the ndimensional delta function is the product measure of the 1dimensional delta functions in each variable separately. Thus, formally, with x = (x_{1}, x_{2}, ..., x_{n}), one has^{[26]}

[math]\displaystyle{ \delta(\mathbf{x}) = \delta(x_1)\,\delta(x_2)\cdots\delta(x_n). }[/math]
(
)
The delta function can also be defined in the sense of distributions exactly as above in the onedimensional case.^{[27]} However, despite widespread use in engineering contexts, (2) should be manipulated with care, since the product of distributions can only be defined under quite narrow circumstances.^{[28]}^{[29]}
The notion of a Dirac measure makes sense on any set.^{[30]} Thus if X is a set, x_{0} ∈ X is a marked point, and Σ is any sigma algebra of subsets of X, then the measure defined on sets A ∈ Σ by
[math]\displaystyle{ \delta_{x_0}(A)=\begin{cases} 1 &\text{if }x_0\in A\\ 0 &\text{if }x_0\notin A \end{cases} }[/math]
is the delta measure or unit mass concentrated at x_{0}.
Another common generalization of the delta function is to a differentiable manifold where most of its properties as a distribution can also be exploited because of the differentiable structure. The delta function on a manifold M centered at the point x_{0} ∈ M is defined as the following distribution:

[math]\displaystyle{ \delta_{x_0}[\varphi] = \varphi(x_0) }[/math]
(
)
for all compactly supported smooth realvalued functions φ on M.^{[31]} A common special case of this construction is a case in which M is an open set in the Euclidean space R^{n}.
On a locally compact Hausdorff space X, the Dirac delta measure concentrated at a point x is the Radon measure associated with the Daniell integral (3) on compactly supported continuous functions φ.^{[32]} At this level of generality, calculus as such is no longer possible, however a variety of techniques from abstract analysis are available. For instance, the mapping [math]\displaystyle{ x_0\mapsto \delta_{x_0} }[/math] is a continuous embedding of X into the space of finite Radon measures on X, equipped with its vague topology. Moreover, the convex hull of the image of X under this embedding is dense in the space of probability measures on X.^{[33]}
Properties
Scaling and symmetry
The delta function satisfies the following scaling property for a nonzero scalar α:^{[34]}
[math]\displaystyle{ \int_{\infty}^\infty \delta(\alpha x)\,dx =\int_{\infty}^\infty \delta(u)\,\frac{du}{\alpha} =\frac{1}{\alpha} }[/math]
and so

[math]\displaystyle{ \delta(\alpha x) = \frac{\delta(x)}{\alpha}. }[/math]
(
)
Scaling property proof: [math]\displaystyle{ \int\limits_{\infty}^{\infty} dx\ g(x) \delta (ax) = \frac{1}{a}\int\limits_{\infty}^{\infty} dx'\ g\left(\frac{x'}{a}\right) \delta (x') }[/math] where a change of variable x′ = ax is used. If a is negative, i.e., a = −a, then [math]\displaystyle{ \int\limits_{\infty}^{\infty} dx\ g(x) \delta (ax) = \frac{1}{\left \vert a \right \vert}\int\limits_{\infty}^{\infty} dx'\ g\left(\frac{x'}{a}\right) \delta (x') = \frac{1}{\left \vert a \right \vert}\int\limits_{\infty}^{\infty} dx'\ g\left(\frac{x'}{a}\right) \delta (x') = \frac{1}{\left \vert a \right \vert}g(0). }[/math] Thus, [math]\displaystyle{ \delta (ax) = \frac{1}{\left \vert a \right \vert} \delta(x) }[/math].
In particular, the delta function is an even distribution (symmetry), in the sense that
[math]\displaystyle{ \delta(x) = \delta(x) }[/math]
which is homogeneous of degree −1.
Algebraic properties
The distributional product of δ with x is equal to zero:
[math]\displaystyle{ x\,\delta(x) = 0. }[/math]
More generally, [math]\displaystyle{ (xa)^n\delta(xa) =0 }[/math] for all positive integers [math]\displaystyle{ n }[/math].
Conversely, if xf(x) = xg(x), where f and g are distributions, then
[math]\displaystyle{ f(x) = g(x) +c \delta(x) }[/math]
for some constant c.^{[35]}
Translation
The integral of the timedelayed Dirac delta is^{[36]}
[math]\displaystyle{ \int_{\infty}^\infty f(t) \,\delta(tT)\,dt = f(T). }[/math]
This is sometimes referred to as the sifting property^{[37]} or the sampling property.^{[38]} The delta function is said to "sift out" the value of f(t) at t = T.^{[39]}
It follows that the effect of convolving a function f(t) with the timedelayed Dirac delta [math]\displaystyle{ \delta_T(t) = \delta(tT) }[/math] is to timedelay f(t) by the same amount:
[math]\displaystyle{ \begin{align} (f * \delta_T)(t) \ &\stackrel{\mathrm{def}}{=}\ \int_{\infty}^\infty f(\tau)\, \delta(tT\tau) \, d\tau \\ &= \int_{\infty}^\infty f(\tau) \,\delta(\tau(tT)) \,d\tau \qquad \text{since}~ \delta(x) = \delta(x) ~~ \text{by (4)}\\ &= f(tT). \end{align} }[/math]
The sifting property holds under the precise condition that f be a tempered distribution (see the discussion of the Fourier transform below). As a special case, for instance, we have the identity (understood in the distribution sense)
[math]\displaystyle{ \int_{\infty}^\infty \delta (\xix) \delta(x\eta) \,dx = \delta(\eta\xi). }[/math]
Composition with a function
More generally, the delta distribution may be composed with a smooth function g(x) in such a way that the familiar change of variables formula holds, that
[math]\displaystyle{ \int_{\R} \delta\bigl(g(x)\bigr) f\bigl(g(x)\bigr) \leftg'(x)\right dx = \int_{g(\R)} \delta(u)\,f(u)\,du }[/math]
provided that g is a continuously differentiable function with g′ nowhere zero.^{[40]} That is, there is a unique way to assign meaning to the distribution [math]\displaystyle{ \delta\circ g }[/math] so that this identity holds for all compactly supported test functions f. Therefore, the domain must be broken up to exclude the g′ = 0 point. This distribution satisfies δ(g(x)) = 0 if g is nowhere zero, and otherwise if g has a real root at x_{0}, then
[math]\displaystyle{ \delta(g(x)) = \frac{\delta(xx_0)}{g'(x_0)}. }[/math]
It is natural therefore to define the composition δ(g(x)) for continuously differentiable functions g by
[math]\displaystyle{ \delta(g(x)) = \sum_i \frac{\delta(xx_i)}{g'(x_i)} }[/math]
where the sum extends over all roots (i.e., all the different ones) of g(x), which are assumed to be simple. Thus, for example
[math]\displaystyle{ \delta\left(x^2\alpha^2\right) = \frac{1}{2\alpha} \Big[\delta\left(x+\alpha\right)+\delta\left(x\alpha\right)\Big]. }[/math]
In the integral form, the generalized scaling property may be written as
[math]\displaystyle{ \int_{\infty}^\infty f(x) \, \delta(g(x)) \, dx = \sum_{i}\frac{f(x_i)}{g'(x_i)}. }[/math]
Indefinite integral
For a constant [math]\displaystyle{ a \isin \mathbb{R} }[/math] and a "wellbehaved" arbitrary realvalued function y(x), [math]\displaystyle{ \displaystyle{\int}y(x)\delta(xa)dx = y(a)H(xa) + c, }[/math] where H(x) is the Heaviside step function and c is an integration constant.
Properties in n dimensions
The delta distribution in an ndimensional space satisfies the following scaling property instead, [math]\displaystyle{ \delta(\alpha\mathbf{x}) = \alpha^{n}\delta(\mathbf{x}) ~, }[/math] so that δ is a homogeneous distribution of degree −n.
Under any reflection or rotation ρ, the delta function is invariant, [math]\displaystyle{ \delta(\rho \mathbf{x}) = \delta(\mathbf{x})~. }[/math]
As in the onevariable case, it is possible to define the composition of δ with a biLipschitz function^{[41]} g: R^{n} → R^{n} uniquely so that the identity [math]\displaystyle{ \int_{\R^n} \delta(g(\mathbf{x}))\, f(g(\mathbf{x}))\left\det g'(\mathbf{x})\right d\mathbf{x} = \int_{g(\R^n)} \delta(\mathbf{u}) f(\mathbf{u})\,d\mathbf{u} }[/math] for all compactly supported functions f.
Using the coarea formula from geometric measure theory, one can also define the composition of the delta function with a submersion from one Euclidean space to another one of different dimension; the result is a type of current. In the special case of a continuously differentiable function g : R^{n} → R such that the gradient of g is nowhere zero, the following identity holds^{[42]} [math]\displaystyle{ \int_{\R^n} f(\mathbf{x}) \, \delta(g(\mathbf{x})) \,d\mathbf{x} = \int_{g^{1}(0)}\frac{f(\mathbf{x})}{\mathbf{\nabla}g}\,d\sigma(\mathbf{x}) }[/math] where the integral on the right is over g^{−1}(0), the (n − 1)dimensional surface defined by g(x) = 0 with respect to the Minkowski content measure. This is known as a simple layer integral.
More generally, if S is a smooth hypersurface of R^{n}, then we can associate to S the distribution that integrates any compactly supported smooth function g over S: [math]\displaystyle{ \delta_S[g] = \int_S g(\mathbf{s})\,d\sigma(\mathbf{s}) }[/math]
where σ is the hypersurface measure associated to S. This generalization is associated with the potential theory of simple layer potentials on S. If D is a domain in R^{n} with smooth boundary S, then δ_{S} is equal to the normal derivative of the indicator function of D in the distribution sense,
[math]\displaystyle{ \int_{\R^n}g(\mathbf{x})\,\frac{\partial 1_D(\mathbf{x})}{\partial n}\,d\mathbf{x}=\int_S\,g(\mathbf{s})\, d\sigma(\mathbf{s}), }[/math]
where n is the outward normal.^{[43]}^{[44]} For a proof, see e.g. the article on the surface delta function.
In three dimensions, the delta function is represented in spherical coordinates by:
[math]\displaystyle{ \delta(\mathbf{r}\mathbf{r}_0) = \begin{cases} \displaystyle\frac{1}{r^2\sin\theta}\delta(rr_0) \delta(\theta\theta_0)\delta(\phi\phi_0)& x_0,y_0,z_0 \ne 0 \\ \displaystyle\frac{1}{2\pi r^2\sin\theta}\delta(rr_0) \delta(\theta\theta_0)& x_0=y_0=0,\ z_0 \ne 0 \\ \displaystyle\frac{1}{4\pi r^2}\delta(rr_0) & x_0=y_0=z_0 = 0 \end{cases} }[/math]
Fourier transform
The delta function is a tempered distribution, and therefore it has a welldefined Fourier transform. Formally, one finds^{[45]}
[math]\displaystyle{ \widehat{\delta}(\xi)=\int_{\infty}^\infty e^{2\pi i x \xi} \,\delta(x)dx = 1. }[/math]
Properly speaking, the Fourier transform of a distribution is defined by imposing selfadjointness of the Fourier transform under the duality pairing [math]\displaystyle{ \langle\cdot,\cdot\rangle }[/math] of tempered distributions with Schwartz functions. Thus [math]\displaystyle{ \widehat{\delta} }[/math] is defined as the unique tempered distribution satisfying
[math]\displaystyle{ \langle\widehat{\delta},\varphi\rangle = \langle\delta,\widehat{\varphi}\rangle }[/math]
for all Schwartz functions φ. And indeed it follows from this that [math]\displaystyle{ \widehat{\delta}=1. }[/math]
As a result of this identity, the convolution of the delta function with any other tempered distribution S is simply S:
[math]\displaystyle{ S*\delta = S. }[/math]
That is to say that δ is an identity element for the convolution on tempered distributions, and in fact, the space of compactly supported distributions under convolution is an associative algebra with identity the delta function. This property is fundamental in signal processing, as convolution with a tempered distribution is a linear timeinvariant system, and applying the linear timeinvariant system measures its impulse response. The impulse response can be computed to any desired degree of accuracy by choosing a suitable approximation for δ, and once it is known, it characterizes the system completely. See LTI system theory § Impulse response and convolution.
The inverse Fourier transform of the tempered distribution f(ξ) = 1 is the delta function. Formally, this is expressed as [math]\displaystyle{ \int_{\infty}^\infty 1 \cdot e^{2\pi i x\xi}\,d\xi = \delta(x) }[/math] and more rigorously, it follows since [math]\displaystyle{ \langle 1, \widehat{f}\rangle = f(0) = \langle\delta,f\rangle }[/math] for all Schwartz functions f.
In these terms, the delta function provides a suggestive statement of the orthogonality property of the Fourier kernel on R. Formally, one has [math]\displaystyle{ \int_{\infty}^\infty e^{i 2\pi \xi_1 t} \left[e^{i 2\pi \xi_2 t}\right]^*\,dt = \int_{\infty}^\infty e^{i 2\pi (\xi_2  \xi_1) t} \,dt = \delta(\xi_2  \xi_1). }[/math]
This is, of course, shorthand for the assertion that the Fourier transform of the tempered distribution [math]\displaystyle{ f(t) = e^{i2\pi\xi_1 t} }[/math] is [math]\displaystyle{ \widehat{f}(\xi_2) = \delta(\xi_1\xi_2) }[/math] which again follows by imposing selfadjointness of the Fourier transform.
By analytic continuation of the Fourier transform, the Laplace transform of the delta function is found to be^{[46]} [math]\displaystyle{ \int_{0}^{\infty}\delta(ta)\,e^{st} \, dt=e^{sa}. }[/math]
Derivatives
The derivative of the Dirac delta distribution, denoted δ′ and also called the Dirac delta prime or Dirac delta derivative as described in Laplacian of the indicator, is defined on compactly supported smooth test functions φ by^{[47]} [math]\displaystyle{ \delta'[\varphi] = \delta[\varphi']=\varphi'(0). }[/math]
The first equality here is a kind of integration by parts, for if δ were a true function then [math]\displaystyle{ \int_{\infty}^\infty \delta'(x)\varphi(x)\,dx = \delta(x)\varphi(x)_{\infty}^{\infty} \int_{\infty}^\infty \delta(x) \varphi'(x)\,dx = \int_{\infty}^\infty \delta(x) \varphi'(x)\,dx = \varphi'(0). }[/math]
By mathematical induction, the kth derivative of δ is defined similarly as the distribution given on test functions by
[math]\displaystyle{ \delta^{(k)}[\varphi] = (1)^k \varphi^{(k)}(0). }[/math]
In particular, δ is an infinitely differentiable distribution.
The first derivative of the delta function is the distributional limit of the difference quotients:^{[48]} [math]\displaystyle{ \delta'(x) = \lim_{h\to 0} \frac{\delta(x+h)\delta(x)}{h}. }[/math]
More properly, one has [math]\displaystyle{ \delta' = \lim_{h\to 0} \frac{1}{h}(\tau_h\delta  \delta) }[/math] where τ_{h} is the translation operator, defined on functions by τ_{h}φ(x) = φ(x + h), and on a distribution S by [math]\displaystyle{ (\tau_h S)[\varphi] = S[\tau_{h}\varphi]. }[/math]
In the theory of electromagnetism, the first derivative of the delta function represents a point magnetic dipole situated at the origin. Accordingly, it is referred to as a dipole or the doublet function.^{[49]}
The derivative of the delta function satisfies a number of basic properties, including:^{[50]} [math]\displaystyle{ \begin{align} \delta'(x) &= \delta'(x) \\ x\delta'(x) &= \delta(x) \end{align} }[/math] which can be shown by applying a test function and integrating by parts.
The latter of these properties can also be demonstrated by applying distributional derivative definition, Liebniz 's theorem and linearity of inner product:^{[51]}
[math]\displaystyle{ \begin{align} \langle x\delta', \varphi \rangle \, &= \, \langle \delta', x\varphi \rangle \, = \, \langle\delta,(x\varphi)'\rangle \, = \,  \langle \delta, x'\varphi + x\varphi'\rangle \, = \,  \langle \delta, x'\varphi\rangle  \langle\delta, x\varphi'\rangle \, = \,  x'(0)\varphi(0)  x(0)\varphi'(0) \\ &= \, x'(0) \langle \delta , \varphi \rangle  x(0) \langle \delta, \varphi' \rangle \, = \, x'(0) \langle \delta,\varphi\rangle + x(0) \langle \delta', \varphi \rangle \, = \, \langle x(0)\delta'  x'(0)\delta, \varphi \rangle \\ \Longrightarrow x(t)\delta'(t) &= x(0)\delta'(t)  x'(0)\delta(t) = x'(0)\delta(t) = \delta(t) \end{align} }[/math]
Furthermore, the convolution of δ′ with a compactlysupported, smooth function f is
[math]\displaystyle{ \delta'*f = \delta*f' = f', }[/math]
which follows from the properties of the distributional derivative of a convolution.
Higher dimensions
More generally, on an open set U in the ndimensional Euclidean space [math]\displaystyle{ \mathbb{R}^n }[/math], the Dirac delta distribution centered at a point a ∈ U is defined by^{[52]} [math]\displaystyle{ \delta_a[\varphi]=\varphi(a) }[/math] for all [math]\displaystyle{ \varphi \in C_c^\infty(U) }[/math], the space of all smooth functions with compact support on U. If [math]\displaystyle{ \alpha = (\alpha_1, \ldots, \alpha_n) }[/math] is any multiindex with [math]\displaystyle{ \alpha=\alpha_1+\cdots+\alpha_n }[/math] and [math]\displaystyle{ \partial^\alpha }[/math] denotes the associated mixed partial derivative operator, then the αth derivative ∂^{α}δ_{a} of δ_{a} is given by^{[52]}
[math]\displaystyle{ \left\langle \partial^\alpha \delta_{a}, \, \varphi \right\rangle = (1)^{ \alpha } \left\langle \delta_{a}, \partial^{\alpha} \varphi \right\rangle = (1)^{ \alpha } \partial^\alpha \varphi (x) \Big_{x = a} \quad \text{ for all } \varphi \in C_c^\infty(U). }[/math]
That is, the αth derivative of δ_{a} is the distribution whose value on any test function φ is the αth derivative of φ at a (with the appropriate positive or negative sign).
The first partial derivatives of the delta function are thought of as double layers along the coordinate planes. More generally, the normal derivative of a simple layer supported on a surface is a double layer supported on that surface and represents a laminar magnetic monopole. Higher derivatives of the delta function are known in physics as multipoles.
Higher derivatives enter into mathematics naturally as the building blocks for the complete structure of distributions with point support. If S is any distribution on U supported on the set Template:Brace consisting of a single point, then there is an integer m and coefficients c_{α} such that^{[52]}^{[53]} [math]\displaystyle{ S = \sum_{\alpha\le m} c_\alpha \partial^\alpha\delta_a. }[/math]
Representations of the delta function
The delta function can be viewed as the limit of a sequence of functions
[math]\displaystyle{ \delta (x) = \lim_{\varepsilon\to 0^+} \eta_\varepsilon(x), }[/math]
where η_{ε}(x) is sometimes called a nascent delta function. This limit is meant in a weak sense: either that

[math]\displaystyle{ \lim_{\varepsilon\to 0^+} \int_{\infty}^\infty \eta_\varepsilon(x)f(x) \, dx = f(0) }[/math]
(
)
for all continuous functions f having compact support, or that this limit holds for all smooth functions f with compact support. The difference between these two slightly different modes of weak convergence is often subtle: the former is convergence in the vague topology of measures, and the latter is convergence in the sense of distributions.
Approximations to the identity
Typically a nascent delta function η_{ε} can be constructed in the following manner. Let η be an absolutely integrable function on R of total integral 1, and define [math]\displaystyle{ \eta_\varepsilon(x) = \varepsilon^{1} \eta \left (\frac{x}{\varepsilon} \right). }[/math]
In n dimensions, one uses instead the scaling [math]\displaystyle{ \eta_\varepsilon(x) = \varepsilon^{n} \eta \left (\frac{x}{\varepsilon} \right). }[/math]
Then a simple change of variables shows that η_{ε} also has integral 1. One may show that (5) holds for all continuous compactly supported functions f,^{[54]} and so η_{ε} converges weakly to δ in the sense of measures.
The η_{ε} constructed in this way are known as an approximation to the identity.^{[55]} This terminology is because the space L^{1}(R) of absolutely integrable functions is closed under the operation of convolution of functions: f ∗ g ∈ L^{1}(R) whenever f and g are in L^{1}(R). However, there is no identity in L^{1}(R) for the convolution product: no element h such that f ∗ h = f for all f. Nevertheless, the sequence η_{ε} does approximate such an identity in the sense that
[math]\displaystyle{ f*\eta_\varepsilon \to f \quad \text{as }\varepsilon\to 0. }[/math]
This limit holds in the sense of mean convergence (convergence in L^{1}). Further conditions on the η_{ε}, for instance that it be a mollifier associated to a compactly supported function,^{[56]} are needed to ensure pointwise convergence almost everywhere.
If the initial η = η_{1} is itself smooth and compactly supported then the sequence is called a mollifier. The standard mollifier is obtained by choosing η to be a suitably normalized bump function, for instance
[math]\displaystyle{ \eta(x) = \begin{cases} e^{\frac{1}{1x^2}}& \text{if } x \lt 1\\ 0 & \text{if } x\geq 1. \end{cases} }[/math]
In some situations such as numerical analysis, a piecewise linear approximation to the identity is desirable. This can be obtained by taking η_{1} to be a hat function. With this choice of η_{1}, one has
[math]\displaystyle{ \eta_\varepsilon(x) = \varepsilon^{1}\max \left (1\left\frac{x}{\varepsilon}\right,0 \right) }[/math]
which are all continuous and compactly supported, although not smooth and so not a mollifier.
Probabilistic considerations
In the context of probability theory, it is natural to impose the additional condition that the initial η_{1} in an approximation to the identity should be positive, as such a function then represents a probability distribution. Convolution with a probability distribution is sometimes favorable because it does not result in overshoot or undershoot, as the output is a convex combination of the input values, and thus falls between the maximum and minimum of the input function. Taking η_{1} to be any probability distribution at all, and letting η_{ε}(x) = η_{1}(x/ε)/ε as above will give rise to an approximation to the identity. In general this converges more rapidly to a delta function if, in addition, η has mean 0 and has small higher moments. For instance, if η_{1} is the uniform distribution on [math]\displaystyle{ \left[\frac{1}{2},\frac{1}{2}\right] }[/math], also known as the rectangular function, then:^{[57]} [math]\displaystyle{ \eta_\varepsilon(x) = \frac{1}{\varepsilon}\operatorname{rect}\left(\frac{x}{\varepsilon}\right)= \begin{cases} \frac{1}{\varepsilon},&\frac{\varepsilon}{2}\lt x\lt \frac{\varepsilon}{2}, \\ 0, &\text{otherwise}. \end{cases} }[/math]
Another example is with the Wigner semicircle distribution [math]\displaystyle{ \eta_\varepsilon(x)= \begin{cases} \frac{2}{\pi \varepsilon^2}\sqrt{\varepsilon^2  x^2}, & \varepsilon \lt x \lt \varepsilon, \\ 0, & \text{otherwise}. \end{cases} }[/math]
This is continuous and compactly supported, but not a mollifier because it is not smooth.
Semigroups
Nascent delta functions often arise as convolution semigroups.^{[58]} This amounts to the further constraint that the convolution of η_{ε} with η_{δ} must satisfy [math]\displaystyle{ \eta_\varepsilon * \eta_\delta = \eta_{\varepsilon+\delta} }[/math]
for all ε, δ > 0. Convolution semigroups in L^{1} that form a nascent delta function are always an approximation to the identity in the above sense, however the semigroup condition is quite a strong restriction.
In practice, semigroups approximating the delta function arise as fundamental solutions or Green's functions to physically motivated elliptic or parabolic partial differential equations. In the context of applied mathematics, semigroups arise as the output of a linear timeinvariant system. Abstractly, if A is a linear operator acting on functions of x, then a convolution semigroup arises by solving the initial value problem
[math]\displaystyle{ \begin{cases} \dfrac{\partial}{\partial t}\eta(t,x) = A\eta(t,x), \quad t\gt 0 \\[5pt] \displaystyle\lim_{t\to 0^+} \eta(t,x) = \delta(x) \end{cases} }[/math]
in which the limit is as usual understood in the weak sense. Setting η_{ε}(x) = η(ε, x) gives the associated nascent delta function.
Some examples of physically important convolution semigroups arising from such a fundamental solution include the following.
The heat kernel
The heat kernel, defined by
[math]\displaystyle{ \eta_\varepsilon(x) = \frac{1}{\sqrt{2\pi\varepsilon}} \mathrm{e}^{\frac{x^2}{2\varepsilon}} }[/math]
represents the temperature in an infinite wire at time t > 0, if a unit of heat energy is stored at the origin of the wire at time t = 0. This semigroup evolves according to the onedimensional heat equation:
[math]\displaystyle{ \frac{\partial u}{\partial t} = \frac{1}{2}\frac{\partial^2 u}{\partial x^2}. }[/math]
In probability theory, η_{ε}(x) is a normal distribution of variance ε and mean 0. It represents the probability density at time t = ε of the position of a particle starting at the origin following a standard Brownian motion. In this context, the semigroup condition is then an expression of the Markov property of Brownian motion.
In higherdimensional Euclidean space R^{n}, the heat kernel is [math]\displaystyle{ \eta_\varepsilon = \frac{1}{(2\pi\varepsilon)^{n/2}}\mathrm{e}^{\frac{x\cdot x}{2\varepsilon}}, }[/math] and has the same physical interpretation, mutatis mutandis. It also represents a nascent delta function in the sense that η_{ε} → δ in the distribution sense as ε → 0.
The Poisson kernel
The Poisson kernel [math]\displaystyle{ \eta_\varepsilon(x) = \frac{1}{\pi}\mathrm{Im}\left\{\frac{1}{x\mathrm{i}\varepsilon}\right\}=\frac{1}{\pi} \frac{\varepsilon}{\varepsilon^2 + x^2}=\frac{1}{2\pi}\int_{\infty}^{\infty}\mathrm{e}^{\mathrm{i} \xi x\varepsilon \xi}\,d\xi }[/math]
is the fundamental solution of the Laplace equation in the upper halfplane.^{[59]} It represents the electrostatic potential in a semiinfinite plate whose potential along the edge is held at fixed at the delta function. The Poisson kernel is also closely related to the Cauchy distribution and Epanechnikov and Gaussian kernel functions.^{[60]} This semigroup evolves according to the equation [math]\displaystyle{ \frac{\partial u}{\partial t} = \left (\frac{\partial^2}{\partial x^2} \right)^{\frac{1}{2}}u(t,x) }[/math]
where the operator is rigorously defined as the Fourier multiplier [math]\displaystyle{ \mathcal{F}\left[\left(\frac{\partial^2}{\partial x^2} \right)^{\frac{1}{2}}f\right](\xi) = 2\pi\xi\mathcal{F}f(\xi). }[/math]
Oscillatory integrals
In areas of physics such as wave propagation and wave mechanics, the equations involved are hyperbolic and so may have more singular solutions. As a result, the nascent delta functions that arise as fundamental solutions of the associated Cauchy problems are generally oscillatory integrals. An example, which comes from a solution of the Euler–Tricomi equation of transonic gas dynamics,^{[61]} is the rescaled Airy function [math]\displaystyle{ \varepsilon^{1/3}\operatorname{Ai}\left (x\varepsilon^{1/3} \right). }[/math]
Although using the Fourier transform, it is easy to see that this generates a semigroup in some sense—it is not absolutely integrable and so cannot define a semigroup in the above strong sense. Many nascent delta functions constructed as oscillatory integrals only converge in the sense of distributions (an example is the Dirichlet kernel below), rather than in the sense of measures.
Another example is the Cauchy problem for the wave equation in R^{1+1}:^{[62]} [math]\displaystyle{ \begin{align} c^{2}\frac{\partial^2u}{\partial t^2}  \Delta u &= 0\\ u=0,\quad \frac{\partial u}{\partial t} = \delta &\qquad \text{for }t=0. \end{align} }[/math]
The solution u represents the displacement from equilibrium of an infinite elastic string, with an initial disturbance at the origin.
Other approximations to the identity of this kind include the sinc function (used widely in electronics and telecommunications) [math]\displaystyle{ \eta_\varepsilon(x)=\frac{1}{\pi x}\sin\left(\frac{x}{\varepsilon}\right)=\frac{1}{2\pi}\int_{\frac{1}{\varepsilon}}^{\frac{1}{\varepsilon}} \cos(kx)\,dk }[/math]
and the Bessel function [math]\displaystyle{ \eta_\varepsilon(x) = \frac{1}{\varepsilon}J_{\frac{1}{\varepsilon}} \left(\frac{x+1}{\varepsilon}\right). }[/math]
Plane wave decomposition
One approach to the study of a linear partial differential equation [math]\displaystyle{ L[u]=f, }[/math]
where L is a differential operator on R^{n}, is to seek first a fundamental solution, which is a solution of the equation [math]\displaystyle{ L[u]=\delta. }[/math]
When L is particularly simple, this problem can often be resolved using the Fourier transform directly (as in the case of the Poisson kernel and heat kernel already mentioned). For more complicated operators, it is sometimes easier first to consider an equation of the form [math]\displaystyle{ L[u]=h }[/math]
where h is a plane wave function, meaning that it has the form [math]\displaystyle{ h = h(x\cdot\xi) }[/math]
for some vector ξ. Such an equation can be resolved (if the coefficients of L are analytic functions) by the Cauchy–Kovalevskaya theorem or (if the coefficients of L are constant) by quadrature. So, if the delta function can be decomposed into plane waves, then one can in principle solve linear partial differential equations.
Such a decomposition of the delta function into plane waves was part of a general technique first introduced essentially by Johann Radon, and then developed in this form by Fritz John (1955).^{[63]} Choose k so that n + k is an even integer, and for a real number s, put [math]\displaystyle{ g(s) = \operatorname{Re}\left[\frac{s^k\log(is)}{k!(2\pi i)^n}\right] =\begin{cases} \frac{s^k}{4k!(2\pi i)^{n1}} &n \text{ odd}\\[5pt] \frac{s^k\logs}{k!(2\pi i)^n}&n \text{ even.} \end{cases} }[/math]
Then δ is obtained by applying a power of the Laplacian to the integral with respect to the unit sphere measure dω of g(x · ξ) for ξ in the unit sphere S^{n−1}: [math]\displaystyle{ \delta(x) = \Delta_x^{(n+k)/2} \int_{S^{n1}} g(x\cdot\xi)\,d\omega_\xi. }[/math]
The Laplacian here is interpreted as a weak derivative, so that this equation is taken to mean that, for any test function φ, [math]\displaystyle{ \varphi(x) = \int_{\mathbf{R}^n}\varphi(y)\,dy\,\Delta_x^{\frac{n+k}{2}} \int_{S^{n1}} g((xy)\cdot\xi)\,d\omega_\xi. }[/math]
The result follows from the formula for the Newtonian potential (the fundamental solution of Poisson's equation). This is essentially a form of the inversion formula for the Radon transform because it recovers the value of φ(x) from its integrals over hyperplanes. For instance, if n is odd and k = 1, then the integral on the right hand side is [math]\displaystyle{ \begin{align} & c_n \Delta^{\frac{n+1}{2}}_x\iint_{S^{n1}} \varphi(y)(yx) \cdot \xi \, d\omega_\xi \, dy \\[5pt] & \qquad = c_n \Delta^{(n+1)/2}_x \int_{S^{n1}} \, d\omega_\xi \int_{\infty}^\infty p R\varphi(\xi,p+x\cdot\xi)\,dp \end{align} }[/math]
where Rφ(ξ, p) is the Radon transform of φ: [math]\displaystyle{ R\varphi(\xi,p) = \int_{x\cdot\xi=p} f(x)\,d^{n1}x. }[/math]
An alternative equivalent expression of the plane wave decomposition is:^{[64]} [math]\displaystyle{ \delta(x) = \begin{cases} \frac{(n1)!}{(2\pi i)^n}\displaystyle\int_{S^{n1}}(x\cdot\xi)^{n} \, d\omega_\xi & n\text{ even} \\ \frac{1}{2(2\pi i)^{n1}}\displaystyle\int_{S^{n1}}\delta^{(n1)}(x\cdot\xi)\,d\omega_\xi & n\text{ odd}. \end{cases} }[/math]
Fourier kernels
In the study of Fourier series, a major question consists of determining whether and in what sense the Fourier series associated with a periodic function converges to the function. The nth partial sum of the Fourier series of a function f of period 2π is defined by convolution (on the interval [−π,π]) with the Dirichlet kernel: [math]\displaystyle{ D_N(x) = \sum_{n=N}^N e^{inx} = \frac{\sin\left(\left(N+\frac12\right)x\right)}{\sin(x/2)}. }[/math] Thus, [math]\displaystyle{ s_N(f)(x) = D_N*f(x) = \sum_{n=N}^N a_n e^{inx} }[/math] where [math]\displaystyle{ a_n = \frac{1}{2\pi}\int_{\pi}^\pi f(y)e^{iny}\,dy. }[/math] A fundamental result of elementary Fourier series states that the Dirichlet kernel restricted to the interval [−π,π] tends to a multiple of the delta function as N → ∞. This is interpreted in the distribution sense, that [math]\displaystyle{ s_N(f)(0) = \int_{\pi}^{\pi} D_N(x)f(x)\,dx \to 2\pi f(0) }[/math] for every compactly supported smooth function f. Thus, formally one has [math]\displaystyle{ \delta(x) = \frac1{2\pi} \sum_{n=\infty}^\infty e^{inx} }[/math] on the interval [−π,π].
Despite this, the result does not hold for all compactly supported continuous functions: that is D_{N} does not converge weakly in the sense of measures. The lack of convergence of the Fourier series has led to the introduction of a variety of summability methods to produce convergence. The method of Cesàro summation leads to the Fejér kernel^{[65]}
[math]\displaystyle{ F_N(x) = \frac1N\sum_{n=0}^{N1} D_n(x) = \frac{1}{N}\left(\frac{\sin \frac{Nx}{2}}{\sin \frac{x}{2}}\right)^2. }[/math]
The Fejér kernels tend to the delta function in a stronger sense that^{[66]}
[math]\displaystyle{ \int_{\pi}^{\pi} F_N(x)f(x)\,dx \to 2\pi f(0) }[/math]
for every compactly supported continuous function f. The implication is that the Fourier series of any continuous function is Cesàro summable to the value of the function at every point.
Hilbert space theory
The Dirac delta distribution is a densely defined unbounded linear functional on the Hilbert space L^{2} of squareintegrable functions. Indeed, smooth compactly supported functions are dense in L^{2}, and the action of the delta distribution on such functions is welldefined. In many applications, it is possible to identify subspaces of L^{2} and to give a stronger topology on which the delta function defines a bounded linear functional.
Sobolev spaces
The Sobolev embedding theorem for Sobolev spaces on the real line R implies that any squareintegrable function f such that
[math]\displaystyle{ \f\_{H^1}^2 = \int_{\infty}^\infty \widehat{f}(\xi)^2 (1+\xi^2)\,d\xi \lt \infty }[/math]
is automatically continuous, and satisfies in particular
[math]\displaystyle{ \delta[f]=f(0) \lt C \f\_{H^1}. }[/math]
Thus δ is a bounded linear functional on the Sobolev space H^{1}. Equivalently δ is an element of the continuous dual space H^{−1} of H^{1}. More generally, in n dimensions, one has δ ∈ H^{−s}(R^{n}) provided s > n/2.
Spaces of holomorphic functions
In complex analysis, the delta function enters via Cauchy's integral formula, which asserts that if D is a domain in the complex plane with smooth boundary, then
[math]\displaystyle{ f(z) = \frac{1}{2\pi i} \oint_{\partial D} \frac{f(\zeta)\,d\zeta}{\zetaz},\quad z\in D }[/math]
for all holomorphic functions f in D that are continuous on the closure of D. As a result, the delta function δ_{z} is represented in this class of holomorphic functions by the Cauchy integral:
[math]\displaystyle{ \delta_z[f] = f(z) = \frac{1}{2\pi i} \oint_{\partial D} \frac{f(\zeta)\,d\zeta}{\zetaz}. }[/math]
Moreover, let H^{2}(∂D) be the Hardy space consisting of the closure in L^{2}(∂D) of all holomorphic functions in D continuous up to the boundary of D. Then functions in H^{2}(∂D) uniquely extend to holomorphic functions in D, and the Cauchy integral formula continues to hold. In particular for z ∈ D, the delta function δ_{z} is a continuous linear functional on H^{2}(∂D). This is a special case of the situation in several complex variables in which, for smooth domains D, the Szegő kernel plays the role of the Cauchy integral.^{[67]}
Resolutions of the identity
Given a complete orthonormal basis set of functions Template:Brace in a separable Hilbert space, for example, the normalized eigenvectors of a compact selfadjoint operator, any vector f can be expressed as [math]\displaystyle{ f = \sum_{n=1}^\infty \alpha_n \varphi_n. }[/math] The coefficients {α_{n}} are found as [math]\displaystyle{ \alpha_n = \langle \varphi_n, f \rangle, }[/math] which may be represented by the notation: [math]\displaystyle{ \alpha_n = \varphi_n^\dagger f, }[/math] a form of the bra–ket notation of Dirac.^{[68]} Adopting this notation, the expansion of f takes the dyadic form:^{[69]}
[math]\displaystyle{ f = \sum_{n=1}^\infty \varphi_n \left ( \varphi_n^\dagger f \right). }[/math]
Letting I denote the identity operator on the Hilbert space, the expression
[math]\displaystyle{ I = \sum_{n=1}^\infty \varphi_n \varphi_n^\dagger, }[/math]
is called a resolution of the identity. When the Hilbert space is the space L^{2}(D) of squareintegrable functions on a domain D, the quantity:
[math]\displaystyle{ \varphi_n \varphi_n^\dagger, }[/math]
is an integral operator, and the expression for f can be rewritten
[math]\displaystyle{ f(x) = \sum_{n=1}^\infty \int_D\, \left( \varphi_n (x) \varphi_n^*(\xi)\right) f(\xi) \, d \xi. }[/math]
The righthand side converges to f in the L^{2} sense. It need not hold in a pointwise sense, even when f is a continuous function. Nevertheless, it is common to abuse notation and write
[math]\displaystyle{ f(x) = \int \, \delta(x\xi) f (\xi)\, d\xi, }[/math]
resulting in the representation of the delta function:^{[70]}
[math]\displaystyle{ \delta(x\xi) = \sum_{n=1}^\infty \varphi_n (x) \varphi_n^*(\xi). }[/math]
With a suitable rigged Hilbert space (Φ, L^{2}(D), Φ*) where Φ ⊂ L^{2}(D) contains all compactly supported smooth functions, this summation may converge in Φ*, depending on the properties of the basis φ_{n}. In most cases of practical interest, the orthonormal basis comes from an integral or differential operator, in which case the series converges in the distribution sense.^{[71]}
Infinitesimal delta functions
Cauchy used an infinitesimal α to write down a unit impulse, infinitely tall and narrow Diractype delta function δ_{α} satisfying [math]\displaystyle{ \int F(x)\delta_\alpha(x) \,dx = F(0) }[/math] in a number of articles in 1827.^{[72]} Cauchy defined an infinitesimal in Cours d'Analyse (1827) in terms of a sequence tending to zero. Namely, such a null sequence becomes an infinitesimal in Cauchy's and Lazare Carnot's terminology.
Nonstandard analysis allows one to rigorously treat infinitesimals. The article by (Yamashita 2007) contains a bibliography on modern Dirac delta functions in the context of an infinitesimalenriched continuum provided by the hyperreals. Here the Dirac delta can be given by an actual function, having the property that for every real function F one has [math]\displaystyle{ \int F(x)\delta_\alpha(x) \, dx = F(0) }[/math] as anticipated by Fourier and Cauchy.
Dirac comb
A socalled uniform "pulse train" of Dirac delta measures, which is known as a Dirac comb, or as the Sha distribution, creates a sampling function, often used in digital signal processing (DSP) and discrete time signal analysis. The Dirac comb is given as the infinite sum, whose limit is understood in the distribution sense,
[math]\displaystyle{ \operatorname{\text{Ш}}(x) = \sum_{n=\infty}^\infty \delta(xn), }[/math]
which is a sequence of point masses at each of the integers.
Up to an overall normalizing constant, the Dirac comb is equal to its own Fourier transform. This is significant because if f is any Schwartz function, then the periodization of f is given by the convolution [math]\displaystyle{ (f * \operatorname{\text{Ш}})(x) = \sum_{n=\infty}^\infty f(xn). }[/math] In particular, [math]\displaystyle{ (f*\operatorname{\text{Ш}})^\wedge = \widehat{f}\widehat{\operatorname{\text{Ш}}} = \widehat{f}\operatorname{\text{Ш}} }[/math] is precisely the Poisson summation formula.^{[73]}^{[74]} More generally, this formula remains to be true if f is a tempered distribution of rapid descent or, equivalently, if [math]\displaystyle{ \widehat{f} }[/math] is a slowly growing, ordinary function within the space of tempered distributions.
Sokhotski–Plemelj theorem
The Sokhotski–Plemelj theorem, important in quantum mechanics, relates the delta function to the distribution p.v. 1/x, the Cauchy principal value of the function 1/x, defined by
[math]\displaystyle{ \left\langle\operatorname{p.v.}\frac{1}{x}, \varphi\right\rangle = \lim_{\varepsilon\to 0^+}\int_{x\gt \varepsilon} \frac{\varphi(x)}{x}\,dx. }[/math]
Sokhotsky's formula states that^{[75]}
[math]\displaystyle{ \lim_{\varepsilon\to 0^+} \frac{1}{x\pm i\varepsilon} = \operatorname{p.v.}\frac{1}{x} \mp i\pi\delta(x), }[/math]
Here the limit is understood in the distribution sense, that for all compactly supported smooth functions f,
[math]\displaystyle{ \int_{\infty}^{\infty}\lim_{\varepsilon\to0^{+}}\frac{f(x)}{x\pm i\varepsilon}\,dx=\mp i\pi f(0)+\lim_{\varepsilon\to0^{+}}\int_{x\gt \varepsilon}\frac{f(x)}{x}\,dx. }[/math]
Relationship to the Kronecker delta
The Kronecker delta δ_{ij} is the quantity defined by
[math]\displaystyle{ \delta_{ij} = \begin{cases} 1 & i=j\\ 0 &i\not=j \end{cases} }[/math]
for all integers i, j. This function then satisfies the following analog of the sifting property: if a_{i} (for i in the set of all integers) is any doubly infinite sequence, then
[math]\displaystyle{ \sum_{i=\infty}^\infty a_i \delta_{ik}=a_k. }[/math]
Similarly, for any real or complex valued continuous function f on R, the Dirac delta satisfies the sifting property
[math]\displaystyle{ \int_{\infty}^\infty f(x)\delta(xx_0)\,dx=f(x_0). }[/math]
This exhibits the Kronecker delta function as a discrete analog of the Dirac delta function.^{[76]}
Applications
Probability theory
In probability theory and statistics, the Dirac delta function is often used to represent a discrete distribution, or a partially discrete, partially continuous distribution, using a probability density function (which is normally used to represent absolutely continuous distributions). For example, the probability density function f(x) of a discrete distribution consisting of points x = Template:Brace, with corresponding probabilities p_{1}, ..., p_{n}, can be written as
[math]\displaystyle{ f(x) = \sum_{i=1}^n p_i \delta(xx_i). }[/math]
As another example, consider a distribution in which 6/10 of the time returns a standard normal distribution, and 4/10 of the time returns exactly the value 3.5 (i.e. a partly continuous, partly discrete mixture distribution). The density function of this distribution can be written as
[math]\displaystyle{ f(x) = 0.6 \, \frac {1}{\sqrt{2\pi}} e^{\frac{x^2}{2}} + 0.4 \, \delta(x3.5). }[/math]
The delta function is also used to represent the resulting probability density function of a random variable that is transformed by continuously differentiable function. If Y = g(X) is a continuous differentiable function, then the density of Y can be written as
[math]\displaystyle{ f_Y(y) = \int_{\infty}^{+\infty} f_X(x) \delta(yg(x)) \,dx. }[/math]
The delta function is also used in a completely different way to represent the local time of a diffusion process (like Brownian motion). The local time of a stochastic process B(t) is given by [math]\displaystyle{ \ell(x,t) = \int_0^t \delta(xB(s))\,ds }[/math] and represents the amount of time that the process spends at the point x in the range of the process. More precisely, in one dimension this integral can be written [math]\displaystyle{ \ell(x,t) = \lim_{\varepsilon\to 0^+}\frac{1}{2\varepsilon}\int_0^t \mathbf{1}_{[x\varepsilon,x+\varepsilon]}(B(s))\,ds }[/math] where [math]\displaystyle{ \mathbf{1}_{[x\varepsilon,x+\varepsilon]} }[/math] is the indicator function of the interval [math]\displaystyle{ [x\varepsilon,x+\varepsilon]. }[/math]
Quantum mechanics
The delta function is expedient in quantum mechanics. The wave function of a particle gives the probability amplitude of finding a particle within a given region of space. Wave functions are assumed to be elements of the Hilbert space L^{2} of squareintegrable functions, and the total probability of finding a particle within a given interval is the integral of the magnitude of the wave function squared over the interval. A set Template:Brace of wave functions is orthonormal if they are normalized by
[math]\displaystyle{ \langle\varphi_n \mid \varphi_m\rangle = \delta_{nm} }[/math]
where δ is the Kronecker delta. A set of orthonormal wave functions is complete in the space of squareintegrable functions if any wave function ψ⟩ can be expressed as a linear combination of the Template:Brace with complex coefficients:
[math]\displaystyle{ \psi = \sum c_n \varphi_n, }[/math]
with c_{n} = ⟨φ_{n}ψ⟩. Complete orthonormal systems of wave functions appear naturally as the eigenfunctions of the Hamiltonian (of a bound system) in quantum mechanics that measures the energy levels, which are called the eigenvalues. The set of eigenvalues, in this case, is known as the spectrum of the Hamiltonian. In bra–ket notation, as above, this equality implies the resolution of the identity:
[math]\displaystyle{ I = \sum \varphi_n\rangle\langle\varphi_n. }[/math]
Here the eigenvalues are assumed to be discrete, but the set of eigenvalues of an observable may be continuous rather than discrete. An example is the position observable, Qψ(x) = xψ(x). The spectrum of the position (in one dimension) is the entire real line and is called a continuous spectrum. However, unlike the Hamiltonian, the position operator lacks proper eigenfunctions. The conventional way to overcome this shortcoming is to widen the class of available functions by allowing distributions as well: that is, to replace the Hilbert space of quantum mechanics with an appropriate rigged Hilbert space.^{[77]} In this context, the position operator has a complete set of eigendistributions, labeled by the points y of the real line, given by
[math]\displaystyle{ \varphi_y(x) = \delta(xy). }[/math]
The eigenfunctions of position are denoted by φ_{y} = y⟩ in Dirac notation, and are known as position eigenstates.
Similar considerations apply to the eigenstates of the momentum operator, or indeed any other selfadjoint unbounded operator P on the Hilbert space, provided the spectrum of P is continuous and there are no degenerate eigenvalues. In that case, there is a set Ω of real numbers (the spectrum), and a collection φ_{y} of distributions indexed by the elements of Ω, such that
[math]\displaystyle{ P\varphi_y = y\varphi_y. }[/math]
That is, φ_{y} are the eigenvectors of P. If the eigenvectors are normalized so that
[math]\displaystyle{ \langle \varphi_y,\varphi_{y'}\rangle = \delta(yy') }[/math]
in the distribution sense, then for any test function ψ,
[math]\displaystyle{ \psi(x) = \int_\Omega c(y) \varphi_y(x) \, dy }[/math]
where c(y) = ⟨ψ, φ_{y}⟩. That is, as in the discrete case, there is a resolution of the identity
[math]\displaystyle{ I = \int_\Omega \varphi_y\rangle\, \langle\varphi_y\,dy }[/math]
where the operatorvalued integral is again understood in the weak sense. If the spectrum of P has both continuous and discrete parts, then the resolution of the identity involves a summation over the discrete spectrum and an integral over the continuous spectrum.
The delta function also has many more specialized applications in quantum mechanics, such as the delta potential models for a single and double potential well.
Structural mechanics
The delta function can be used in structural mechanics to describe transient loads or point loads acting on structures. The governing equation of a simple mass–spring system excited by a sudden force impulse I at time t = 0 can be written
[math]\displaystyle{ m \frac{d^2 \xi}{dt^2} + k \xi = I \delta(t), }[/math]
where m is the mass, ξ is the deflection, and k is the spring constant.
As another example, the equation governing the static deflection of a slender beam is, according to Euler–Bernoulli theory,
[math]\displaystyle{ EI \frac{d^4 w}{dx^4} = q(x), }[/math]
where EI is the bending stiffness of the beam, w is the deflection, x is the spatial coordinate, and q(x) is the load distribution. If a beam is loaded by a point force F at x = x_{0}, the load distribution is written
[math]\displaystyle{ q(x) = F \delta(xx_0). }[/math]
As the integration of the delta function results in the Heaviside step function, it follows that the static deflection of a slender beam subject to multiple point loads is described by a set of piecewise polynomials.
Also, a point moment acting on a beam can be described by delta functions. Consider two opposing point forces F at a distance d apart. They then produce a moment M = Fd acting on the beam. Now, let the distance d approach the limit zero, while M is kept constant. The load distribution, assuming a clockwise moment acting at x = 0, is written
[math]\displaystyle{ \begin{align} q(x) &= \lim_{d \to 0} \Big( F \delta(x)  F \delta(xd) \Big) \\[4pt] &= \lim_{d \to 0} \left( \frac{M}{d} \delta(x)  \frac{M}{d} \delta(xd) \right) \\[4pt] &= M \lim_{d \to 0} \frac{\delta(x)  \delta(x  d)}{d}\\[4pt] &= M \delta'(x). \end{align} }[/math]
Point moments can thus be represented by the derivative of the delta function. Integration of the beam equation again results in piecewise polynomial deflection.
See also
Notes
 ↑ atis 2013, unit impulse.
 ↑ Arfken & Weber 2000, p. 84.
 ↑ ^{3.0} ^{3.1} Dirac 1930, §22 The δ function.
 ↑ Gelfand & Shilov 1966–1968, Volume I, §1.1.
 ↑ Zhao, JiCheng (20110505) (in en). Methods for Phase Diagram Determination. Elsevier. ISBN 9780080549965. https://books.google.com/books?id=blZYGDREpk8C&pg=PA174.
 ↑ Fourier, JB (1822). The Analytical Theory of Heat (English translation by Alexander Freeman, 1878 ed.). The University Press. p. [1]., cf. https://books.google.com/books?id=N8EAAAAYAAJ&pg=PA449 and pp. 546–551. Original French text.
 ↑ Komatsu, Hikosaburo (2002). "Fourier's hyperfunctions and Heaviside's pseudodifferential operators". Microlocal Analysis and Complex Fourier Analysis. World Scientific. p. [2]. ISBN 9789812381613. https://books.google.com/books?id=8GwKzEemrIcC.
 ↑ MyintU., Tyn; Debnath, Lokenath (2007). Linear Partial Differential Equations for Scientists And Engineers (4th ed.). Springer. p. [3]. ISBN 9780817643935. https://books.google.com/books?id=Zbz5_UvERIIC.
 ↑ Debnath, Lokenath; Bhatta, Dambaru (2007). Integral Transforms And Their Applications (2nd ed.). CRC Press. p. [4]. ISBN 9781584885757. https://books.google.com/books?id=WbZcqdvCEfwC.
 ↑ GrattanGuinness, Ivor (2009). Convolutions in French Mathematics, 1800–1840: From the Calculus and Mechanics to Mathematical Analysis and Mathematical Physics, Volume 2. Birkhäuser. p. 653. ISBN 9783764322380. https://books.google.com/books?id=_GgioErrbW8C.
 ↑ See, for example, Cauchy, AugustinLouis (17891857) Auteur du texte (1882–1974). "Des intégrales doubles qui se présentent sous une forme indéterminèe" (in EN). Oeuvres complètes d'Augustin Cauchy. Série 1, tome 1 / publiées sous la direction scientifique de l'Académie des sciences et sous les auspices de M. le ministre de l'Instruction publique.... http://gallica.bnf.fr/ark:/12148/bpt6k90181x/f387.
 ↑ Mitrović, Dragiša; Žubrinić, Darko (1998). Fundamentals of Applied Functional Analysis: Distributions, Sobolev Spaces. CRC Press. p. 62. ISBN 9780582246942. https://books.google.com/books?id=Od5BxTEN0VsC.
 ↑ Kracht, Manfred; Kreyszig, Erwin (1989). "On singular integral operators and generalizations". in Themistocles M. Rassias. Topics in Mathematical Analysis: A Volume Dedicated to the Memory of A.L. Cauchy. World Scientific. p. https://books.google.com/books?id=xIsPrSiDlZIC&pg=PA553 553]. ISBN 9789971506667. https://books.google.com/books?id=xIsPrSiDlZIC.
 ↑ Laugwitz 1989, p. 230.
 ↑ A more complete historical account can be found in van der Pol & Bremmer 1987, §V.4.
 ↑ Dirac, P. A. M. (January 1927). "The physical interpretation of the quantum dynamics" (in en). Proceedings of the Royal Society of London. Series A, Containing Papers of a Mathematical and Physical Character 113 (765): 621–641. doi:10.1098/rspa.1927.0012. ISSN 09501207. Bibcode: 1927RSPSA.113..621D.
 ↑ Gelfand & Shilov 1966–1968, Volume I, §1.1, p. 1.
 ↑ Dirac 1930, p. 63.
 ↑ Rudin 1966, §1.20
 ↑ Hewitt & Stromberg 1963, §19.61.
 ↑ Driggers 2003, p. 2321 See also Bracewell 1986, Chapter 5 for a different interpretation. Other conventions for the assigning the value of the Heaviside function at zero exist, and some of these are not consistent with what follows.
 ↑ Hewitt & Stromberg 1963, §9.19.
 ↑ Hazewinkel 2011, p. 41.
 ↑ Strichartz 1994, §2.2.
 ↑ Hörmander 1983, Theorem 2.1.5.
 ↑ Bracewell 1986, Chapter 5.
 ↑ Hörmander 1983, §3.1.
 ↑ Strichartz 1994, §2.3.
 ↑ Hörmander 1983, §8.2.
 ↑ Rudin 1966, §1.20.
 ↑ Dieudonné 1972, §17.3.3.
 ↑ Krantz, Steven G.; Parks, Harold R. (20081215) (in en). Geometric Integration Theory. Springer Science & Business Media. ISBN 9780817646790. https://books.google.com/books?id=X_BKmVphIcsC&q.
 ↑ Federer 1969, §2.5.19.
 ↑ Strichartz 1994, Problem 2.6.2.
 ↑ Vladimirov 1971, Chapter 2, Example 3(d).
 ↑ Rottwitt, Karsten; TidemandLichtenberg, Peter (20141211) (in en). Nonlinear Optics: Principles and Applications. CRC Press. p. [5] 276. ISBN 9781466565838. https://books.google.com/books?id=G1jSBQAAQBAJ.
 ↑ Weisstein, Eric W.. "Sifting Property". http://mathworld.wolfram.com/SiftingProperty.html.
 ↑ Karris, Steven T. (2003) (in en). Signals and Systems with MATLAB Applications. Orchard Publications. p. 15. ISBN 9780970951168. https://books.google.com/books?id=f0RdM1zv_dkC.
 ↑ Roden, Martin S. (20140517) (in en). Introduction to Communication Theory. Elsevier. p. [6]. ISBN 9781483145563. https://books.google.com/books?id=YEKeBQAAQBAJ.
 ↑ Gelfand & Shilov 1966–1968, Vol. 1, §II.2.5.
 ↑ Further refinement is possible, namely to submersions, although these require a more involved change of variables formula.
 ↑ Hörmander 1983, §6.1.
 ↑ Lange 2012, pp.29–30.
 ↑ Gelfand & Shilov 1966–1968, p. 212.
 ↑ The numerical factors depend on the conventions for the Fourier transform.
 ↑ Bracewell 1986.
 ↑ Gelfand & Shilov 1966–1968, p. 26.
 ↑ Gelfand & Shilov 1966–1968, §2.1.
 ↑ Weisstein, Eric W.. "Doublet Function". http://mathworld.wolfram.com/DoubletFunction.html.
 ↑ Bracewell 2000, p. 86.
 ↑ "Gugo82's comment on the distributional derivative of Dirac's delta". 12 September 2010. https://www.matematicamente.it/forum/viewtopic.php?f=36&t=62388&start=10#wrap.
 ↑ ^{52.0} ^{52.1} ^{52.2} Hörmander 1983, p. 56.
 ↑ Rudin 1991, Theorem 6.25.
 ↑ Stein & Weiss 1971, Theorem 1.18.
 ↑ Rudin 1991, §II.6.31.
 ↑ More generally, one only needs η = η_{1} to have an integrable radially symmetric decreasing rearrangement.
 ↑ Saichev & Woyczyński 1997, §1.1 The "delta function" as viewed by a physicist and an engineer, p. 3.
 ↑ Milovanović, Gradimir V.; Rassias, Michael Th (20140708) (in en). Analytic Number Theory, Approximation Theory, and Special Functions: In Honor of Hari M. Srivastava. Springer. p. 748. ISBN 9781493902583. https://books.google.com/books?id=4U5BQAAQBAJ.
 ↑ Stein & Weiss 1971, §I.1.
 ↑ Mader, Heidy M. (2006) (in en). Statistics in Volcanology. Geological Society of London. p. 81. ISBN 9781862392083. https://books.google.com/books?id=e5Y_RRPxdyYC.
 ↑ Vallée & Soares 2004, §7.2.
 ↑ Hörmander 1983, §7.8.
 ↑ Courant & Hilbert 1962, §14.
 ↑ Gelfand & Shilov 1966–1968, I, §3.10.
 ↑ Lang 1997, p. 312.
 ↑ In the terminology of (Lang 1997), the Fejér kernel is a Dirac sequence, whereas the Dirichlet kernel is not.
 ↑ Hazewinkel 1995, p. 357.
 ↑ The development of this section in bra–ket notation is found in (Levin 2002)
 ↑ Davis & Thomson 2000, Perfect operators, p.344.
 ↑ Davis & Thomson 2000, Equation 8.9.11, p. 344.
 ↑ de la Madrid, Bohm & Gadella 2002.
 ↑ Laugwitz 1989.
 ↑ Córdoba 1988.
 ↑ Hörmander 1983, §7.2.
 ↑ Vladimirov 1971, §5.7.
 ↑ Hartmann 1997, pp. 154–155.
 ↑ Isham 1995, §6.2.
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External links
 Hazewinkel, Michiel, ed. (2001), "Deltafunction", Encyclopedia of Mathematics, Springer Science+Business Media B.V. / Kluwer Academic Publishers, ISBN 9781556080104, https://www.encyclopediaofmath.org/index.php?title=p/d030950
 KhanAcademy.org video lesson
 The Dirac Delta function, a tutorial on the Dirac delta function.
 Video Lectures – Lecture 23, a lecture by Arthur Mattuck.
 The Dirac delta measure is a hyperfunction
 We show the existence of a unique solution and analyze a finite element approximation when the source term is a Dirac delta measure
 NonLebesgue measures on R. LebesgueStieltjes measure, Dirac delta measure.
Original source: https://en.wikipedia.org/wiki/Dirac delta function.
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