What Are the Radii of Convergence for a Laurent Series Around a Singular Point?

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Discussion Overview

The discussion revolves around determining the radii of convergence for a Laurent series centered at a singular point, specifically analyzing the function f(z) = (z*sin(z))/(2z-1) around the point z=1/2. Participants explore the implications of poles and the nature of singularities on the inner and outer radii of convergence, as well as the process of finding residues.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants assert that since z=1/2 is a pole, the inner radius of convergence is zero and the outer radius is infinite.
  • Others clarify that the outer radius being infinite is not solely due to the pole but can be inferred from the convergence properties of the sine series.
  • A participant questions whether a function like exp(1/z) has an inner radius greater than zero due to having infinite negative terms.
  • There is a discussion about finding the residue at the pole z=1/2, with some suggesting that the function should be expressed in terms of (z-1/2).
  • One participant expresses confusion about obtaining a -1 order term in the series expansion for sine around z=1/2, leading to a discussion about the nature of singularities.
  • Another participant explains that the function 1/(z-i) is already in the form of a Laurent series and discusses the implications of expanding it around different points.
  • There is a distinction made between poles and essential singularities, with participants debating the conditions under which each occurs.

Areas of Agreement / Disagreement

Participants express differing views on the implications of having infinite negative terms in a Laurent series and the conditions for determining inner radii of convergence. The discussion remains unresolved regarding the exact nature of singularities and their impact on the series expansions.

Contextual Notes

Some participants note that the inner radius can only be greater than zero if the Laurent series does not terminate at negative directions, while others challenge this notion. The discussion includes various assumptions about the nature of singularities and the convergence of series, which are not fully resolved.

naggy
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I'm puzzled by one thing concerning Laurent series.

If I have a series, for example f(z) =(z*sinz)/(2z-1) and I'm supposed to make a laurent series of f about the point z=1/2.

Now, what would the inner and outer radius of convergence be?

I would say that since z=1/2 is a pole, the inner radius is zero and the outer radius infinite?

If not, then how can I see the radius of convergence of a Laurent series?
 
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naggy said:
I would say that since z=1/2 is a pole, the inner radius is zero and the outer radius infinite?

Result is correct, and the first conclusion too. Inner radius can be greater than zero only if Laurent series don't terminate at negative direction. Now the smallest order term in the Laurent series is of order -1, so inner radius is zero.

The outer radius is infinite, but you cannot conclude it from the fact that z=1/2 is a pole. Instead it is seen most easily from the fact, that the series of sine have the factorials 1/n! which make series convergent everywhere.

If not, then how can I see the radius of convergence of a Laurent series?

Most of the time it is best to try to see them by using previous knowledge of already known functions, but when all else fails, the outer and inner radius, [itex]\rh<img src="https://cdn.jsdelivr.net/joypixels/assets/8.0/png/unicode/64/1f635.png" class="smilie smilie--emoji" loading="lazy" width="64" height="64" alt="o_O" title="Er... what? o_O" data-smilie="12"data-shortname="o_O" />[/itex] and [itex]\rho_I[/itex], of a Laurent series

[tex] \sum_{n=-\infty}^{\infty} a_n (z-z_0)^n[/tex]

are given by the formulas

[tex] \rh<img src="https://cdn.jsdelivr.net/joypixels/assets/8.0/png/unicode/64/1f635.png" class="smilie smilie--emoji" loading="lazy" width="64" height="64" alt="o_O" title="Er... what? o_O" data-smilie="12"data-shortname="o_O" /> = \frac{1}{\underset{n\to\infty}{\textrm{lim sup}}\; \sqrt[n]{|a_n|}}[/tex]

[tex] \rho_I = \underset{n\to\infty}{\textrm{lim sup}}\; \sqrt[n]{|a_{-n}|}[/tex]
 
jostpuur said:
Result is correct, and the first conclusion too. Inner radius can be greater than zero only if Laurent series don't terminate at negative direction. Now the smallest order term in the Laurent series is of order -1, so inner radius is zero.

The outer radius is infinite, but you cannot conclude it from the fact that z=1/2 is a pole. Instead it is seen most easily from the fact, that the series of sine have the factorials 1/n! which make series convergent everywhere.
[/tex]

Then for example exp(1/z) has infinite negative terms and so has an inner radius higher than zero?


Another thing. If I wanted to find the residue of the pole(z=1/2) by writing the function as an infinite series, how would I do that? I would have to write it in terms of (z-1/2) right?

I tried doing it for sine about z=1/2 but the the denominator canceled and I did not gera a -1 order term in the series.
 
naggy said:
Then for example exp(1/z) has infinite negative terms and so has an inner radius higher than zero?

No.

This claim is right: If Laurent series has only finite amount of non-zero terms with negative exponent, then the inner radius is zero.

This claim is wrong: If Laurent series has infinite amount of non-zero terms with negative exponent, then the inner radius is greater than zero.

These first claim does not imply the second.

(edit: and my original comment
jostpuur said:
Inner radius can be greater than zero only if Laurent series don't terminate at negative direction.
is equivalent with the first claim)

Another thing. If I wanted to find the residue of the pole(z=1/2) by writing the function as an infinite series, how would I do that? I would have to write it in terms of (z-1/2) right?

Yes. You need to solve the coefficient [itex]a_{-1}[/itex] from the series

[tex] \frac{z\sin(z)}{2z-1} \;=\; \frac{a_{-1}}{z-\frac{1}{2}} \;+\; a_0 \;+\; a_1(z-\frac{1}{2}) \;+\; a_2(z-\frac{1}{2})^2 \;+\; \cdots[/tex]

I tried doing it for sine about z=1/2 but the the denominator canceled and I did not gera a -1 order term in the series.

I believe you made a mistake. [itex]\frac{1}{2}\sin(\frac{1}{2})\neq 0[/itex], so the -1 order term should be there.
 
jostpuur said:
I believe you made a mistake. [itex]\frac{1}{2}\sin(\frac{1}{2})\neq 0[/itex], so the -1 order term should be there.

I don´t understand how that leads to the a-1 term. Is it because then the function would have a rectifiable singularity, that is the limit would exist as z goes to 1/2?

These things are confusing me a bit. For example I don´t get a a-1 term in a function like f(z) = 1/(z-i) if I expand it as a geometric series. Well, I get an a-1 term but an infinite number of negative powers, and that, by definition, should not give me a pole, but something called an essential singularity.

But I KNOW that z=i is a pole, since the function goes to infinity as z->i
 
naggy said:
I don´t understand how that leads to the a-1 term. Is it because then the function would have a rectifiable singularity, that is the limit would exist as z goes to 1/2?

I'm not sure what rectifiable singularity means. If [itex]f(z_0)=0[/itex], then [tex]\frac{f(z)}{z-z_0}[/tex] has a removable singularity at [itex]z_0[/itex], at least. It sounds like you understood this already, but merely weren't sure?

These things are confusing me a bit. For example I don´t get a a-1 term in a function like f(z) = 1/(z-i) if I expand it as a geometric series.

This function already is in the form of Laurent series. It is

[tex] \frac{1}{z-i} = \sum_{n=-\infty}^{\infty} a_n (z-i)^n[/tex]

with coefficients [itex]a_{-1} = 1[/itex] and [itex]a_n = 0[/itex] for [itex]n\neq -1[/itex].

If you did this:

[tex] \frac{1}{z-i} = \frac{i}{1 + iz} = i\sum_{n=0}^{\infty} (-iz)^n = \sum_{n=0}^{\infty} (-1)^n i^{n+1} z^n[/tex]

then you have expanded the function as Laurent series around the point [itex]z=0[/itex], and not around the point [itex]z=i[/itex]. In this case the inner radius of convergence is 0, and outer radius is 1. There does not exist [itex]z^{-1}[/itex] term with non-zero coefficient, because the original function doesn't have singularity at [itex]z=0[/itex]. The singularity is at [itex]z=i[/itex], and it has the effect that the (open) domain of convergence cannot be larger than [itex]\{z\in\mathbb{C}\;|\; |z|<1\}[/itex], because a larger ball would contain the [itex]z=i[/itex]. The singularity prevents the domain of convergence from being larger.

Well, I get an a-1 term but an infinite number of negative powers, and that, by definition, should not give me a pole, but something called an essential singularity.

Now I'm guessing, but do you mean series like this?

[tex] \frac{1}{z-i} = \frac{1}{z} \frac{1}{1 - \frac{i}{z}} = \frac{1}{z} \sum_{n=0}^{\infty} \Big(\frac{i}{z}\Big)^n = \sum_{n=-\infty}^{-1} (-i)^{n+1} z^n[/tex]

Here the function is written as Laurent series around the point [itex]z=0[/itex] so that the (open) domain of convergence is [itex]\{z\in\mathbb{C}\;|\; |z|>1\}[/itex]. That means the inner radius of convergence is 1, and the outer radius is [itex]\infty[/itex]. The original function doesn't have essential singularity at [itex]z=0[/itex] despite these negative powers in this expansion, because now [itex]z=0[/itex] is outside (and not even on the boundary) the domain of convergence. To see what happens at the [itex]z=0[/itex], you need to use the Laurent series which converge for [itex]|z|<1[/itex].
 
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