Difference between revisions of "Delta-function"
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+ | ''-function, Dirac delta-function, \delta(x)'' | ||
− | A function which makes it possible to describe the spatial density of a physical magnitude (mass, charge, intensity of a heat source, force, etc.) which is concentrated or applied at a point | + | A function which makes it possible to describe the spatial density of a physical magnitude (mass, charge, intensity of a heat source, force, etc.) which is concentrated or applied at a point a of a space \mathbf R^n. For instance, using the delta-function the density of a point mass m located at a point a is written as m\delta(x-a). The delta-function may be formally defined by the relation |
− | + | \[\int\limits_{\mathbf R^n}\delta(x-a)f(x)\,dx=f(a)\] | |
− | for any continuous function | + | for any continuous function f. The derivatives \delta^{(k)} of the delta-function may be defined in a similar manner: |
− | + | \[\int\limits_{\mathbf R^n}\delta^k(x-a)f(x)\,dx=(-1)^kf^{(k)}(a)\] | |
− | for the class of functions | + | for the class of functions f that are continuous in \mathbf R^n with derivatives f^{(k)} up to the order k inclusive. The formal operator relations, which are frequently employed, and which express the following properties of the delta-function: |
− | + | \[\delta(-x)=\delta(x);\qquad\delta(cx)=|c|^{-1}\delta(x),\quad c=\mathrm{const},\] | |
− | + | \[x\delta(x)=0;\qquad\delta(x)+x\delta'(x)=0,\] | |
− | etc., should be understood in the sense of the above definitions, i.e. these relations become meaningful only after having been integrated against sufficiently smooth functions. Thus, the delta-function is not an ordinary function in the sense of the classical theory of functions, and is defined in the theory of generalized functions as a singular [[Generalized function|generalized function]], i.e. as the continuous linear functional in the space of infinitely-differentiable functions | + | etc., should be understood in the sense of the above definitions, i.e. these relations become meaningful only after having been integrated against sufficiently smooth functions. Thus, the delta-function is not an ordinary function in the sense of the classical theory of functions, and is defined in the theory of generalized functions as a singular [[Generalized function|generalized function]], i.e. as the continuous linear functional in the space of infinitely-differentiable functions f of compact support, assigning to f its value at zero: $(\delta,f)=f(0)$. |
====Comments==== | ====Comments==== | ||
− | The Dirac delta-function is the derivative (in the sense of distributions or generalized functions) of the [[Heaviside function]] (Heaviside distribution) | + | The Dirac delta-function is the derivative (in the sense of distributions or generalized functions) of the [[Heaviside function]] (Heaviside distribution) h, defined by $h(x)=0$ for $x<0$, $h(x)=1 for x>0$ (the value at zero does not matter; as usual for a distribution it suffices for it to be defined apart from a set of measure zero). |
====References==== | ====References==== | ||
<table><TR><TD valign="top">[a1]</TD> <TD valign="top"> L. Schwartz, "Théorie des distributions" , '''1–2''' , Hermann (1966) {{MR|0209834}} {{ZBL|0149.09501}} </TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top"> I.M. Gel'fand, G.E. Shilov, "Generalized functions" , '''1. Properties and operations''' , Acad. Press (1964) (Translated from Russian) {{MR|435831}} {{ZBL|0115.33101}} </TD></TR></table> | <table><TR><TD valign="top">[a1]</TD> <TD valign="top"> L. Schwartz, "Théorie des distributions" , '''1–2''' , Hermann (1966) {{MR|0209834}} {{ZBL|0149.09501}} </TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top"> I.M. Gel'fand, G.E. Shilov, "Generalized functions" , '''1. Properties and operations''' , Acad. Press (1964) (Translated from Russian) {{MR|435831}} {{ZBL|0115.33101}} </TD></TR></table> |
Latest revision as of 22:12, 31 December 2018
\delta-function, Dirac delta-function, \delta(x)
A function which makes it possible to describe the spatial density of a physical magnitude (mass, charge, intensity of a heat source, force, etc.) which is concentrated or applied at a point a of a space \mathbf R^n. For instance, using the delta-function the density of a point mass m located at a point a is written as m\delta(x-a). The delta-function may be formally defined by the relation
\int\limits_{\mathbf R^n}\delta(x-a)f(x)\,dx=f(a)
for any continuous function f. The derivatives \delta^{(k)} of the delta-function may be defined in a similar manner:
\int\limits_{\mathbf R^n}\delta^k(x-a)f(x)\,dx=(-1)^kf^{(k)}(a)
for the class of functions f that are continuous in \mathbf R^n with derivatives f^{(k)} up to the order k inclusive. The formal operator relations, which are frequently employed, and which express the following properties of the delta-function:
\delta(-x)=\delta(x);\qquad\delta(cx)=|c|^{-1}\delta(x),\quad c=\mathrm{const},
x\delta(x)=0;\qquad\delta(x)+x\delta'(x)=0,
etc., should be understood in the sense of the above definitions, i.e. these relations become meaningful only after having been integrated against sufficiently smooth functions. Thus, the delta-function is not an ordinary function in the sense of the classical theory of functions, and is defined in the theory of generalized functions as a singular generalized function, i.e. as the continuous linear functional in the space of infinitely-differentiable functions f of compact support, assigning to f its value at zero: (\delta,f)=f(0).
Comments
The Dirac delta-function is the derivative (in the sense of distributions or generalized functions) of the Heaviside function (Heaviside distribution) h, defined by h(x)=0 for x<0, h(x)=1 for x>0 (the value at zero does not matter; as usual for a distribution it suffices for it to be defined apart from a set of measure zero).
References
[a1] | L. Schwartz, "Théorie des distributions" , 1–2 , Hermann (1966) MR0209834 Zbl 0149.09501 |
[a2] | I.M. Gel'fand, G.E. Shilov, "Generalized functions" , 1. Properties and operations , Acad. Press (1964) (Translated from Russian) MR435831 Zbl 0115.33101 |
Delta-function. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Delta-function&oldid=30696