The beta function
is the name used by Legendre and Whittaker and Watson (1990) for the beta
integral (also called the Eulerian integral of the first kind). It is defined
by
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(1)
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The beta function
is implemented in the Wolfram Language
as Beta[a,
b].
To derive the integral representation of the beta function, write the product of two factorials as
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(2)
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Now, let ,
, so
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(3)
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(4)
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Transforming to polar coordinates with ,
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(5)
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(6)
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(7)
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(8)
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The beta function is then defined by
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(9)
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(10)
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Rewriting the arguments then gives the usual form for the beta function,
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(11)
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(12)
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By symmetry,
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(13)
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The general trigonometric form is
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(14)
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Equation (14) can be transformed to an integral over polynomials by letting ,
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(15)
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(16)
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(17)
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(18)
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For any
with
,
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(19)
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(Krantz 1999, p. 158).
To put it in a form which can be used to derive the Legendre duplication formula, let , so
and
, and
|
(20)
| |||
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(21)
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To put it in a form which can be used to develop integral representations of the Bessel functions and hypergeometric
function, let ,
so
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(22)
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In particular, the substitution and the reflection
relation give, for
,
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(23)
| |||
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(24)
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Derivatives of the beta function are given by
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(25)
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(26)
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(27)
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(28)
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where
is the polygamma function.
Various identities can be derived using the Gauss multiplication formula
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(29)
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(30)
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Additional identities include
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(31)
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(32)
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(33)
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(34)
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(35)
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If is a positive
integer, then
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(36)
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In addition,
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(37)
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|
(38)
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The beta function is also given by the product
|
(39)
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(Andrews et al. 1999, p. 8).
Gosper gave the general formulas
|
(40)
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for odd , and
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(41)
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which are an immediate consequence of the analogous identities for gamma functions. Plugging
and
into the above give the special cases
|
(42)
|
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(43)
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