Gauss's Integral Form of Digamma Function
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Theorem
Let $z$ be a complex number with a positive real part.
Then:
- $\ds \map \psi z = \int_0^\infty \paren {\frac {e^{-t} } t - \frac {e^{-z t} } {1 - e^{-t} } } \rd t$
where $\psi$ is the digamma function.
Proof
From Extension of Harmonic Number to Non-Integer Argument, we have:
- $\map H x = \gamma + \dfrac {\map {\Gamma'} {x + 1} } {\map \Gamma {x + 1} }$
which is equivalent to:
- $\ds \map \psi z = -\gamma + H_{z - 1}$
We aim to demonstrate:
- $\ds \int_0^\infty \paren {\frac {e^{-t} } t - \frac {e^{-z t} } {1 - e^{-t} } } \rd t = -\gamma + H_{z - 1}$
We have:
\(\ds \map \psi z\) | \(=\) | \(\ds \int_0^\infty \paren {\frac {e^{-t} } t - \frac {e^{-z t} } {1 - e^{-t} } } \rd t\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \int_0^\infty \frac {e^{-t} } t \rd t - \int_0^\infty \frac {e^{-z t} } {1 - e^{-t} } \rd t\) | Linear Combination of Integrals | |||||||||||
\(\ds \) | \(=\) | \(\ds \int_0^\infty \frac {e^{-t} } t \rd t - \int_0^\infty \frac {e^{-t} } {1 - e^{-t} } \rd t + \int_0^\infty \frac {e^{-t} } {1 - e^{-t} } \rd t - \int_0^\infty \frac {e^{-z t} } {1 - e^{-t} } \rd t\) | adding $0$ | |||||||||||
\(\ds \) | \(=\) | \(\ds \int_0^\infty \frac {e^{-t} } t \rd t - \int_0^\infty \frac {e^{-t} } {1 - e^{-t} } \rd t + \int_0^\infty \frac {e^{-t} - e^{-t z } } {1 - e^{-t} } \rd t\) | Linear Combination of Integrals | |||||||||||
\(\ds \) | \(=\) | \(\ds \int_0^\infty \frac {e^{-t} } t \rd t - \int_0^\infty \frac {e^{-t} } {1 - e^{-t} } \times \frac {e^t} {e^t} \rd t + \int_0^\infty \frac {e^{-t} - e^{-t z } } {1 - e^{-t} } \rd t\) | multiplying by $1$ | |||||||||||
\(\ds \) | \(=\) | \(\ds \int_0^\infty \frac {e^{-t} } t \rd t - \int_0^\infty \frac 1 {e^t - 1 } \rd t + \int_0^\infty \frac {e^{-t} - e^{-t z } } {1 - e^{-t} } \rd t\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \int_0^\infty \paren {\frac {e^{-t} } t - \frac 1 {e^t - 1 } } \rd t + \int_0^\infty \frac {e^{-t} - e^{-t z } } {1 - e^{-t} } \rd t\) | Linear Combination of Integrals | |||||||||||
\(\ds \) | \(=\) | \(\ds -\gamma + \int_0^\infty \paren {\frac {1 - e^{-t\paren {z - 1} } } {1 - e^{-t} } } e^{-t} \rd t\) | Definite Integral to Infinity of Reciprocal of Exponential of x minus One minus Exponential of -x over x |
Let:
\(\ds u\) | \(=\) | \(\ds e^{-t}\) | Integration by Substitution | |||||||||||
\(\ds \leadsto \ \ \) | \(\ds \frac {\d u} {\d t}\) | \(=\) | \(\ds -e^{-t}\) | Derivative of Exponential Function: Corollary 1 |
We also have:
\(\ds \lim_{t \mathop \to 0} e^{-t}\) | \(=\) | \(\ds 1\) | Exponential of Zero | |||||||||||
\(\ds \lim_{t \mathop \to \infty} e^{-t}\) | \(=\) | \(\ds 0\) | Complex Exponential Tends to Zero |
Then:
\(\ds \map \psi z\) | \(=\) | \(\ds -\gamma + \int_{\to 1}^{\to 0} \paren {\dfrac {1 - u^{z - 1} } {1 - u} } \paren {-\rd u}\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds -\gamma + \int_{\to 0}^{\to 1} \paren {\dfrac {1 - u^{z - 1} } {1 - u} } \rd u\) | reversing limits of integration | |||||||||||
\(\ds \) | \(=\) | \(\ds -\gamma + \int_{\to 0}^{\to 1} \sum_{k \mathop = 0}^{z - 2} u^k\) | Sum of Geometric Sequence | |||||||||||
\(\ds \) | \(=\) | \(\ds -\gamma + \sum_{k \mathop = 0}^{z - 2} \int_{\to 0}^{\to 1} u^k\) | Tonelli's Theorem | |||||||||||
\(\ds \) | \(=\) | \(\ds -\gamma + \sum_{k \mathop = 0}^{z - 2} \intlimits {\dfrac {u^{k + 1} } {k + 1} } 0 1\) | Integral of Power | |||||||||||
\(\ds \) | \(=\) | \(\ds -\gamma + \sum_{k \mathop = 0}^{z - 2} \frac 1 {k + 1}\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds -\gamma + \sum_{k \mathop = 1}^{z - 1} \frac 1 k\) | reindexing the sum | |||||||||||
\(\ds \) | \(=\) | \(\ds -\gamma + H_{z - 1}\) | Definition of Harmonic Numbers |
$\blacksquare$
Source of Name
This entry was named for Carl Friedrich Gauss.
Also see
- Definite Integral to Infinity of Reciprocal of Exponential of x minus One minus Exponential of -x over x
- Dirichlet's Integral Form of Digamma Function
Sources
- 1920: E.T. Whittaker and G.N. Watson: A Course of Modern Analysis (3rd ed.): $12.3$: Gauss's expression for the logarithmic derivate of the Gamma function as an infinite integral