Reflection relation for gamma function: Difference between revisions
(New page: ==Statement== Let <math>\Gamma</math> denote the gamma function. Then, for any <math>z</math> that is not an integer, we have: <math>\Gamma(z)\Gamma(1-z) = \frac{\pi}{\sin (\pi z)}</...) |
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* [[Recurrence relation for gamma function]]: This shows that it suffices to prove the result for <math>\operatorname{Re}(z) \in (0,1)</math> | * [[Recurrence relation for gamma function]]: This shows that it suffices to prove the result for <math>\operatorname{Re}(z) \in (0,1)</math> | ||
* The following identity, for <math>0 < \operatorname{Re}(a) < 1</math>: | |||
<math>\int_0^1 \frac{v^{a-1}}{1 + v} = \frac{\pi{\sin \pi z}</math> | |||
==Proof== | |||
===Proof of the integration identity=== | |||
Pick a branch of the logarithm that is slit along the positive real axis, and thus rewrite: | |||
<math>v^{a - 1} = e^{(a - 1)\log v}</math> | |||
Where the branch of logarithm is chosen so that the approach to the positive real axis from the upper half-plane side is the usual logarithm. | |||
Next, apply the [[keyhole contour integration method]] to compute this integral. The inner and outer circle integrals approach zero, and if we define: | |||
<math>I ::= \int_0^1 \frac{v^{a-1}}{1 + v}</math> | |||
Then, we'll obtain: | |||
<math>I(e^{2\pi i (a - 1)} - 1) = 2\pi i \operatorname{res}(\frac{e^{(a - 1)\log v}}{1 + v}; -1)</math> | |||
The residue at <math>-1</math> is simple <math>e^{\pi i (a - 1)}</math> and simplifying the expression, we obtain the required expression for <math>I</math>. | |||
===Proving the result using the integration identity=== |
Revision as of 19:08, 1 May 2008
Statement
Let denote the gamma function. Then, for any that is not an integer, we have:
Facts used
- Recurrence relation for gamma function: This shows that it suffices to prove the result for
- The following identity, for :
Failed to parse (syntax error): {\displaystyle \int_0^1 \frac{v^{a-1}}{1 + v} = \frac{\pi{\sin \pi z}}
Proof
Proof of the integration identity
Pick a branch of the logarithm that is slit along the positive real axis, and thus rewrite:
Where the branch of logarithm is chosen so that the approach to the positive real axis from the upper half-plane side is the usual logarithm.
Next, apply the keyhole contour integration method to compute this integral. The inner and outer circle integrals approach zero, and if we define:
Then, we'll obtain:
The residue at is simple and simplifying the expression, we obtain the required expression for .