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Mathematical Methods for Physicists: A concise introduction - Site Map

Mathematical Methods for Physicists: A concise introduction - Site Map

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THE GAMMA AND BETA FUNCTIONS<br />

When ˆ n, a positive integer, repeated application of Eq. (2.40) and use of Eq.<br />

(2.39) gives<br />

…n ‡ 1† ˆn…n† ˆn…n 1†…n 1† ˆ...ˆ n…n 1†3 2 …1†<br />

ˆ n…n 1†3 2 1 ˆ n!:<br />

Thus the gamma function is a generalization of the factorial function. Eq. (2.40)<br />

enables the values of the gamma function <strong>for</strong> any positive value of to be<br />

calculated: thus<br />

… 7 2 †ˆ…5 2 †…5 2 †ˆ…5 2 †…3 2 †…3 2 †ˆ…5 2 †…3 2 †…1 2 †…1 2 †:<br />

p<br />

Write u ˆ‡<br />

x in Eq. (2.38) and we then obtain<br />

so that<br />

…† ˆ2<br />

Z 1<br />

0<br />

0<br />

u 21 e u2 du;<br />

Z 1<br />

… 1 2 †ˆ2 p<br />

e u2 du ˆ :<br />

The function …† has been tabulated <strong>for</strong> values of between 0 and 1.<br />

When 0†: …2:41†<br />

Substituting t ˆ v=…1 ‡ v†, this can be written in the alternative <strong>for</strong>m<br />

B…p; q† ˆ<br />

Z 1<br />

0<br />

v p1 …1 ‡ v† pq dv:<br />

…2:42†<br />

By writing t 0 ˆ 1 t we deduce that B…p; q† ˆB…q; p†.<br />

The beta function can be expressed in terms of gamma functions as follows:<br />

B…p; q† ˆ…p†…q†<br />

…p ‡ q† :<br />

…2:43†<br />

To prove this, write x ˆ at (a > 0) in the integral (2.38) de®ning …†, and it is<br />

straight<strong>for</strong>ward to show that<br />

…†<br />

a <br />

ˆ<br />

Z 1<br />

0<br />

95<br />

e at t 1 dt<br />

…2:44†

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