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Physics LibreTexts

10.3: C- Clinic on the Gamma Function

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The gamma function Γ(s) is defined, for s > 0, by

Γ(s)=0xs1exdx.

Upon seeing any integral, your first thought is to evaluate it. Stay calm. . . first make sure that the integral exists. A quick check shows that the integral above converges when s > 0.

There is no simple formula for the gamma function for arbitrary s. But for s = 1,

Γ(1)=0exdx=ex|0=1.

For s > 1 we may integrate by parts,

0xs1exdx=xs1ex|0+(s1)0xs2exdx,

giving

Γ(s)=(s1)Γ(s1) for s>1.

Apply equation (C.4) repeatedly for n a positive integer,

Γ(n)=(n1)Γ(n1)=(n1)(n2)Γ(n2)=(n1)(n2)21Γ(1)=(n1)!,

to find a relation between the gamma function and the factorial function. Thus the gamma function generalizes the factorial function to non-integer values, and can be used to define the factorial function through

x!=Γ(x+1) for any x>1.

In particular,

0!=Γ(1)=1.

(It is a deep and non-obvious result that the gamma function is in fact the simplest generalization of the factorial function.)

The gamma function can be simplified for half-integral arguments. For example

Γ(12)=0x1/2exdx=0y1ey2(2ydy)=ey2dy=π

where we used the substitution y=x. Thus

Γ(32)=12Γ(12)=π2=(12)!,

Γ(52)=32Γ(32)=34π,

and so forth.


This page titled 10.3: C- Clinic on the Gamma Function is shared under a CC BY-SA license and was authored, remixed, and/or curated by Daniel F. Styer.

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