Laurent series of z^2sin(1/(z-1))

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SUMMARY

The discussion focuses on finding the Laurent series of the function $$z^2 \sin\left(\frac{1}{1-z}\right)$$ for the region $$0 < |z-1| < \infty$$. The user initially transforms the variable to $$w = \frac{1}{z-1}$$ and expands the sine function using its series representation. The challenge arises in combining the resulting series into a single expression due to differing indices for even and odd powers. The solution involves recognizing that the Laurent series can indeed be expressed as a combination of multiple sums, with coefficients organized by parity.

PREREQUISITES
  • Understanding of Laurent series and their applications in complex analysis.
  • Familiarity with Taylor series and sine function expansions.
  • Knowledge of index manipulation in series summation.
  • Proficiency in complex variable transformations, specifically with the substitution $$w = \frac{1}{z-1}$$.
NEXT STEPS
  • Study the properties of Laurent series and their convergence in complex analysis.
  • Learn about Taylor series expansions for trigonometric functions, particularly sine.
  • Explore techniques for manipulating series, including index shifts and combining sums.
  • Investigate the implications of even and odd power series in mathematical analysis.
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Students and professionals in mathematics, particularly those studying complex analysis, series expansions, and anyone working with Laurent series in theoretical or applied contexts.

Arya Prasetya
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Homework Statement



Find Laurent series of $$z^2sin(\frac{1}{1-z})$$ at $$0<\lvert z-1 \rvert<\infty$$

Homework Equations



sine series expansion.

The Attempt at a Solution



At first, it seems pretty elementary since you can set
w=\frac{1}{z-1} and expand at infinity in z, which is 0 in w. Therefore, $$z^2sin(\frac{1}{z-1})=(\frac{1}{w^2}+\frac{2}{w}+1)sin(w)$$
$$=(\frac{1}{w^2}+\frac{2}{w}+1)\sum_{n=0}^\infty\frac{(-1)^nw^{2n+1}}{(2n+1)!}$$
$$=\sum_{n=0}^\infty\frac{(-1)^nw^{2n-1}}{(2n+1)!}+2\sum_{n=0}^\infty\frac{(-1)^nw^{2n}}{(2n+1)!}+\sum_{n=0}^\infty\frac{(-1)^nw^{2n+1}}{(2n+1)!}$$

But now, I am having troubles adjusting the sums so that the coefficients coincide into one series. The problem I have right now is the change of indices. I believe it is possible to do it for the 1st and 3rd term so that it becomes one. However, It might be impossible incorporating the term contributing to even powers of the w into one sum. Is it the case that Laurent series is able to be represented as 2 or more sums and have its coefficient on an even-odd case basis? Have I done something wrong?

Looking forward for the help and thanks in advance.
 
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Arya Prasetya said:

Homework Statement



Find Laurent series of $$z^2sin(\frac{1}{1-z})$$ at $$0<\lvert z-1 \rvert<\infty$$

Homework Equations



sine series expansion.

The Attempt at a Solution



At first, it seems pretty elementary since you can set
w=\frac{1}{z-1} and expand at infinity in z, which is 0 in w. Therefore, $$z^2sin(\frac{1}{z-1})=(\frac{1}{w^2}+\frac{2}{w}+1)sin(w)$$
$$=(\frac{1}{w^2}+\frac{2}{w}+1)\sum_{n=0}^\infty\frac{(-1)^nw^{2n+1}}{(2n+1)!}$$
$$=\sum_{n=0}^\infty\frac{(-1)^nw^{2n-1}}{(2n+1)!}+2\sum_{n=0}^\infty\frac{(-1)^nw^{2n}}{(2n+1)!}+\sum_{n=0}^\infty\frac{(-1)^nw^{2n+1}}{(2n+1)!}$$

But now, I am having troubles adjusting the sums so that the coefficients coincide into one series. The problem I have right now is the change of indices. I believe it is possible to do it for the 1st and 3rd term so that it becomes one. However, It might be impossible incorporating the term contributing to even powers of the w into one sum. Is it the case that Laurent series is able to be represented as 2 or more sums and have its coefficient on an even-odd case basis? Have I done something wrong?

Looking forward for the help and thanks in advance.
It often helps to write down a couple of terms, say from ##w^{-1}## to ##w^3##. Another possibility is to introduce new counters: ##m=2n-1## in the first series, ##m=2n## in the second, and ##m=2n+1## in the third. The second has only even powers, and the first and third have only odd powers, so they can be added. You'll get an extra term for ##w^{-1}## which occurs only once. In the end you'll get something like
$$
a_{-1}w^{-1} + \sum_{m \;even}a_mw^m + \sum_{m \;odd}a_mw^m
$$
which results in ##\sum_{m \geq -1}a_mw^m## with ##a_m =
\begin{cases}
\ldots & \text{if } m = -1 \\
\ldots & \text{if } m \geq 0 \text{ and } m \text{ odd } \\
\ldots & \text{if } m \geq 0 \text{ and } m \text{ even }
\end{cases}##
 
Ahh ok, got it got it, that's what I thought. Thanks for the insight! :)
 

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