Can Euler's Reflection Formula Simplify the POTW #178 Gamma Function Problem?

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    2015
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SUMMARY

The discussion centers on the application of Euler's Reflection Formula to simplify the Problem of the Week (POTW) #178 related to the Gamma function. The integral representation of the Gamma function is presented as $$\frac{1}{\Gamma(s)} = -\frac{1}{2\pi i} \int_\gamma (-z)^{-s}e^{-z}\, dz$$, where the contour $\gamma$ is defined by specific paths in the complex plane. The problem remains unanswered, indicating a need for further exploration and solutions within the mathematical community.

PREREQUISITES
  • Understanding of complex analysis, particularly contour integration.
  • Familiarity with the Gamma function and its properties.
  • Knowledge of Euler's Reflection Formula and its applications.
  • Basic skills in mathematical notation and integral calculus.
NEXT STEPS
  • Study the derivation and applications of Euler's Reflection Formula in detail.
  • Explore advanced techniques in contour integration within complex analysis.
  • Investigate the properties and applications of the Gamma function in various mathematical contexts.
  • Review solutions to similar problems in the Problem of the Week archives for additional insights.
USEFUL FOR

Mathematicians, students of complex analysis, and anyone interested in advanced calculus and the properties of the Gamma function will benefit from this discussion.

Euge
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Here is this week's POTW:

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Show that

$$\frac{1}{\Gamma(s)} = -\frac{1}{2\pi i} \int_\gamma (-z)^{-s}e^{-z}\, dz,$$

where $\gamma$ is a contour which is the union of a line from $+\infty$ to $\epsilon$ (where $\epsilon > 0$), an $\epsilon$-circle about the origin, and a line from $\epsilon$ to $+\infty$.

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Note: If you like, you may use Euler's reflection formula.

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No one answered this week's problem. You can read my solution below.
For $m = 1,2,3,\ldots$, the integrals $\int_{\gamma, |z| \le m} (-z)^{s-1}e^{-z}\, dz$ are entire functions of $s$, and converge uniformly on compact disks, so the limit function

$$\int_{\gamma} (-z)^{s-1}e^{-z}\, dz$$

is entire. This integral does not depend on $\epsilon$, by Cauchy's theorem. Now the integral along the arc of $\gamma$ is negligible as $\epsilon \to 0$. In the upper half of $\gamma$, $\arg(-z) = -\pi$, and in the lower half, $\arg(-z) = \pi$. So the contribution of the rays of $\gamma$ is $$e^{(s-1)\pi i} \int_\epsilon^\infty x^{s-1}e^{-x}\, dx + e^{-(s-1)\pi i} \int_\epsilon^\infty x^{s-1}e^{-x}\, dx = 2i\sin[\pi(s-1)]\int_\epsilon^\infty x^{s-1}e^{-x}\, dx = -2i\sin(\pi s)\int_\epsilon^\infty x^{s-1}e^{-x}\, dx.$$ Since $\int_\epsilon x^{s-1}e^{-x}\, dx \to \Gamma(s)$ as $\epsilon \to 0$ for $\operatorname{Re}(s) > 0$, it follows that

$$\Gamma(s) = -\frac{1}{2i\sin \pi s}\int_\gamma (-z)^{s-1}e^{-z}\, dz$$

for $\operatorname{Re}(s) > 0$. But by the principle of analytic continuation, the above formula holds for all $s\in \Bbb C \setminus \Bbb Z$. Using Euler's reflection formula $\Gamma(s)\Gamma(1 - s) = \pi/\sin(\pi s)$, we deduce

$$\frac{1}{\Gamma(s)} = \frac{i}{2\pi} \int_\gamma (-z)^{-s}e^{-z}\, dz.$$
 

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