Residue of f(z) involving digamma function

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SUMMARY

The residue of the function \( f(z) = \frac{(\psi(-z) + \gamma)}{(z+1)(z+2)^3} \) at the poles \( z = n \) (where \( n \) is a positive integer) is determined to be a simple pole. The digamma function \( \psi(-z) \) contributes to the residue, requiring the expression \( \psi(-z) = (z+n)g(z) \) where \( g(z) \) is analytic at \( z = -n \). For higher order poles, the residue can be calculated using the Harmonic Number \( H_n \), leading to a coefficient of \( 2H_n \) for the squared function \( (\psi(-z) + \gamma)^2 \).

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  • Knowledge of Harmonic Numbers and their significance in series
  • Ability to manipulate limits and series expansions in calculus
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Amad27
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Homework Statement


Find the residue of:

$$f(z) = \frac{(\psi(-z) + \gamma)}{(z+1)(z+2)^3} \space \text{at} \space z=n$$

Where $n$ is every positive integer because those $n$ are the poles of $f(z)$

Homework Equations

The Attempt at a Solution



This is a simple pole, however:

$$\lim_{z \to n} \frac{(z-n)\psi(-z)}{(z+1)(z+2)^3}$$

But this gives 0, which is incorrect?
 
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For n to be a simple pole of ##\psi (-z) ## you will need to be able to express ##\psi (-z) = (z+n)g(z)## where g(z) is analytic at z=-n. Be careful with your signs.
Using the expansion ##\psi (n)+\gamma= \sum_{k=1}^n-1 \frac 1k ## shows that for every positive integer n there will be a simple pole at z=-n, since the sum will include k=0.
 
RUber said:
For n to be a simple pole of ψ(−z)\psi (-z) you will need to be able to express ψ(−z)=(z+n)g(z)\psi (-z) = (z+n)g(z) where g(z) is analytic at z=-n. Be careful with your signs.
Using the expansion ψ(n)+γ=∑nk=1−11k\psi (n)+\gamma= \sum_{k=1}^n-1 \frac 1k shows that for every positive integer n there will be a simple pole at z=-n, since the sum will include k=0.


Yes I see this, but what about higher order poles? consider:

Suppose we are given:

Find the residue at z=n of $$(\psi(-z) + \gamma)^2$$

Where $$\psi(-z)$$ means the digamma function.

$$(\psi(-z) +\gamma)^2 = \left( 1 + \frac{1}{2} + \frac{1}{z} + \frac{1}{3} + \frac{1}{z-1} + \frac{1}{4} + \frac{1}{z-2} + ... + \frac{1}{n} + \frac{1}{z-n} + ... \right)\left( 1 + \frac{1}{2} + \frac{1}{z} + \frac{1}{3} + \frac{1}{z-1} + \frac{1}{4} + \frac{1}{z-2} + ... + \frac{1}{n} + \frac{1}{z-n} + ... \right) $$

We see that we have:

$$\frac{1}{z-n} \cdot \left( 1 + \frac{1}{2} + \frac{1}{3} + ... + \frac{1}{n} + \frac{1}{z-1} + \frac{1}{z-2} + ... + \frac{1}{z-n} \right) $$

The pure coefficient of $$\frac{1}{z-n}$$ is simply:

$$ \left( 1 + \frac{1}{2} + \frac{1}{3} + ... + \frac{1}{n} \right) = H_n$$

Where $$H_n$$ means the Harmonic Number.

But then we also had the other $$\frac{1}{z-n}$$ in the other parentheses so twice this.

$$2 \left( 1 + \frac{1}{2} + \frac{1}{3} + ... + \frac{1}{n} \right) = 2H_n$$

But does finding the coefficient work for higher order residues?

Thanks!
 

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