A mathematical concept generalizing the classical concept of a function. The need for such a generalization arises in many problems in engineering, physics and mathematics. The concept of a generalized function makes it possible to express in a mathematically-correct form such idealized concepts as the density of a material point, a point charge or a point dipole, the (space) density of a simple or double layer, the intensity of an instantaneous source, etc. On the other hand, the concept of a generalized function reflects the fact that in reality a physical quantity cannot be measured at a point; only its mean values over sufficiently small neighbourhoods of a given point can be measured. Thus, the technique of generalized functions serves as a convenient and adequate apparatus for describing the distributions of various physical quantities. Hence generalized functions are also called distributions.
Generalized functions were first introduced at the end of the 1920-s by P.A.M. Dirac (see ) in his research on quantum mechanics, in which he made systematic use of the concept of the -function and its derivatives (see Delta-function). The foundations of the mathematical theory of generalized functions were laid by S.L. Sobolev  in 1936 by solving the Cauchy problem for hyperbolic equations, while in the 1950-s L. Schwartz (see ) gave a systematic account of the theory of generalized functions and indicated many applications. The theory was then intensively developed by many mathematicians and theoretical physicists, mainly in connection with the needs of theoretical and mathematical physics and the theory of differential equations (see –). The theory of generalized functions has made great advances, has numerous applications, and is extensively used in mathematics, physics and engineering.
Formally, a generalized function is defined as a continuous linear functional on some vector space of sufficiently "good" (test) functions ; . An important example of a test space is the space — the collection of -functions on an open set , with compact support in , endowed with the topology of the strong inductive limit (union) of the spaces , , compact, . The space is the collection of -functions with support in , with the topology given by the countable set of norms
An example of a test function in is the "cap functioncap" :
The space of generalized functions is the space dual to ; , . Convergence of a sequence of generalized functions in is defined as weak convergence of functionals in , that is, , as , in means that , as , for all .
For a linear functional on to be a generalized function in , that is, , it is necessary and sufficient that for any open set there exist numbers and such that
If the integer in (1) can be chosen independently of , then the generalized function has finite order; the least such is called the order of in . Thus, by (1), every generalized function has finite order in any relatively compact .
The space is complete: If a sequence of generalized functions , in is such that for any the sequence of numbers converges, then the functional
belongs to .
The simplest examples of generalized functions are those generated by locally integrable functions on :
Generalized functions definable by (2) in terms of locally integrable functions on are called regular generalized functions on ; the remaining generalized functions are called singular. There is a one-to-one correspondence between locally integrable functions on and regular generalized functions on . In this sense, the "ordinary" , that is, locally integrable on , functions are (regular) generalized functions in .
An example of a singular generalized function on is the Dirac -function
It describes the density of a unit mass concentrated at the point . The "cap" (weakly) approximates the -function:
Let and let be a "cap" . Then the function
in is called the regularization of , and , as , in . Moreover, each in is the weak limit of functions in . The latter property is sometimes taken as the starting point for the definition of a generalized function; together with the theorem on the completeness of the space of generalized functions it leads to an equivalent definition of generalized functions .
In general, a generalized function need not have a value at an individual point. Nonetheless, one speaks of a generalized function coinciding with a locally integrable function on an open set: A generalized function coincides on with a locally integrable function on if its restriction to is , that is, in accordance with (2), if
for all . One then says that , . In particular, with one obtains a definition of the vanishing of a generalized function in . The set of points of with the property that does not vanish on any neighbourhood of is called the support of , denoted by (cf. also Support of a generalized function). If and is relatively compact, then is called of compact support in .
The following theorem on piecewise glueing generalized functions holds: Suppose that for each a generalized function in is given, where is a neighbourhood of , so that the elements are compatible, that is, in ; then there exists a generalized function in that coincides with in for all .
Examples of generalized functions.
1) The Dirac -function: .
2) The generalized function , defined by
is called the finite part, or principal value, of the integral of ; . The distribution is singular on , but on the open set it is regular and coincides with .
3) The surface -function. Let be a piecewise-smooth surface and let be a continuous function on . The generalized function is defined by
Here for , and is a singular function. This generalized function describes the space density of masses or charges concentrated on with surface density (density of a simple layer).
Linear operations on generalized functions are introduced as extensions of the corresponding operations on the test functions.
Change of variables.
Let and let be a linear transformation of onto . The generalized function in is defined by
Since the operation is an isomorphism of onto , the operation is an isomorphism of onto . In particular, if , , ( is a similarity (with a reflection if )), then
if ( is a shift by ), then
Formula (3) enables one to define generalized functions that are translation invariant, spherically symmetric, centrally symmetric, homogeneous, periodic, Lorentz invariant, etc.
Let the function have only simple zeros on the line . The function is defined by
6) , .
Let and . The product is defined by
It turns out that , and for ordinary integrable functions coincides with the usual multiplication of the functions and (cf. also Generalized functions, product of).
However, this product operation cannot be extended to arbitrary generalized functions in such a way that it is associative and commutative. In fact, if this could be done, then one obtains a contradiction:
Such a product can be defined for certain classes of generalized functions, but it may fail to be uniquely defined.
Let . The generalized (weak) derivative of ,
of order is defined by
Since the operation is linear and continuous from into , the functional defined by the right-hand side of (4) is a generalized function in . If , then for all with .
The following properties hold: the operation is linear and continuous from into , and any generalized function in is infinitely differentiable (in the generalized sense); the derivative does not depend on the order of differentiation; the Leibniz formula is valid for the differentiation of a product , where ; differentiation does not enlarge the support; for any open set , every generalized function in is a derivative of a continuous function in ; any differential equation , , with constant coefficients can be solved in , if is a convex domain; any generalized function of order with support at the point can be uniquely represented in the form
10) , where is the Heaviside function (jump function):
11) ; describes the charge density of a dipole of moment at the point , oriented along the positive -axis.
12) The normal derivative of the density of a simple layer on an orientable surface is a generalization of :
The generalized function describes the space charge density corresponding to a distribution of dipoles on with moment surface density and oriented along a given direction of the normal to (density of a double layer).
13) The general solution of the equation in the class is , where is an arbitrary constant.
14) The general solution of the equation in the class is .
15) , .
16) The trigonometric series
converges in ; it can be differentiated term by term infinitely many times in .
Cf. also Generalized function, derivative of a.
Let and . Their direct product is defined by the formula
Since the operation is linear and continuous from into , the functional , defined by (5), is a generalized function in . The direct product is a commutative and associative operation, and
A generalized function in does not depend on if it can be represented in the form
in this case one writes .
19) The general solution in of the equation for the vibration of a homogeneous string, , is given by
where and are arbitrary generalized functions in .
Let and be generalized functions in with the property that their direct product can be extended to functions of the form , where runs through , in the following sense: For every sequence of functions in with the properties
(on any compact set), the sequence of numbers has a limit independent of the sequence . This limit is called the convolution of and , and is denoted by . Thus,
The completeness of implies that . As elementary examples show, the convolution does not exist for all pairs and . It does exists if one of the generalized functions is of compact support. If the convolution exists in , then it is commutative, , and the following formulas for the differentiation of a convolution are valid:
hence, from (7),
shows that convolution is a non-associative operation. However, associative (and commutative) convolution algebras exist. By (8), the -function is the identity element in them. For example, a convolution algebra is formed by the set consisting of the generalized functions in with support in a convex acute closed cone with vertex at . One writes:
A generalized function in is called a fundamental solution (point-source function) of a differential operator with constant coefficients if it satisfies the equation
If a fundamental solution of is known, then a solution can be constructed for the equation for those in for which the convolution exists, and this solution is given by .
20) The kernel of a fractional differentiation or integration operator , :
Here , , , , an integer. If , then is the primitive of order for (derivative of order for ).
It is defined on the class of generalized functions of slow growth. The space of test functions consists of the -functions that decrease at infinity together with all their derivatives faster than any power of . The topology of is given by the countable set of norms
Here and , and these imbeddings are continuous. Functions of slow growth that are locally integrable on are in , and define regular functionals on by formula (2).
Every generalized function in is a derivative of a continuous function of slow growth, and so has finite order on .
The Fourier transform of a generalized function in is defined by the equation
is the classical Fourier transform. Since the operation is an isomorphism of onto , the operation is an isomorphism of onto , and the inverse of is given by
The following basic formulas hold for :
if has compact support. If the generalized function is periodic with -period , , then , and it can be expanded in a trigonometric series
converging to in . Here
24) ; in particular, .
25) ; in particular, .
Let the generalized function , where is a closed convex acute cone. Let , where is the cone dual to . The Laplace transform of is defined by
The mapping defines an isomorphism of the convolution algebra onto the algebra consisting of the functions that are holomorphic in the wedge and that satisfy the following growth condition: There exist numbers and such that for any cone (i.e. ) there exists a number such that
The inverse of the Laplace transform is given by the equation
where the right-hand side of (10) is independent of .
The one-to-one correspondence between and given by equations (9) and (10) can be conveniently represented by the following scheme:
in which is called the transform of , and the spectral function of .
Every in the algebra has a boundary value as , , in , related to the spectral function of by the formula according to (9). The following basic formulas hold for the Laplace transform:
27) ; in particular,
|||P.A.M. Dirac, "The principles of quantum mechanics" , Clarendon Press (1947)|
|||S.L. Sobolev, "Méthode nouvelle à résoudre le problème de Cauchy pour les équations linéaires hyperboliques normales" Mat. Sb. , 1 (1936) pp. 39–72|
|||L. Schwartz, "Théorie des distributions" , 1–2 , Hermann (1950–1951)|
|||N.N. Bogolyubov, A.A. Logunov, I.T. Todorov, "Introduction to axiomatic quantum field theory" , Benjamin (1975) (Translated from Russian)|
|||I.M. Gel'fand, G.E. Shilov, "Generalized functions" , 1–5 , Acad. Press (1966–1968) (Translated from Russian)|
|||V.S. Vladimirov, "Equations of mathematical physics" , MIR (1984) (Translated from Russian)|
|||V.S. Vladimirov, "Generalized functions in mathematical physics" , MIR (1979) (Translated from Russian)|
|||P. Antosik, J. Mikusiński, R. Sikorski, "Theory of distributions. The sequential approach" , Elsevier (1973)|
The notation means that the closure is contained in . Usually the support of a function (or distribution) is defined as the closure of the set of points where it is non-zero.
|[a1]||K. Yosida, "Functional analysis" , Springer (1980) pp. Chapt. 8, Sect. 4; 5|
|[a2]||D.S. Jones, "The theory of generalized functions" , Cambridge Univ. Press (1982)|
|[a3]||W. Rudin, "Functional analysis" , McGraw-Hill (1974)|
|[a4]||L.V. Hörmander, "The analysis of linear partial differential operators" , 1 , Springer (1983)|
Generalized function. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Generalized_function&oldid=12767