Holomorphic functions at stationary points

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Discussion Overview

The discussion revolves around the conformal mapping property of holomorphic functions, particularly focusing on how this property breaks down at stationary points. Participants explore the implications of differentiability in complex analysis and the behavior of functions near these critical points.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Ayae expresses interest in understanding the conformal mapping property of holomorphic functions and its breakdown at stationary points, seeking further reading and insights.
  • One participant explains that holomorphic functions are conformal where their derivative is non-zero, using power series expansion to illustrate how the local behavior resembles linear functions when the derivative is non-zero.
  • The same participant notes that if the derivative vanishes, higher order terms dominate, leading to transformations that are not conformal, such as the mapping z to z², which doubles angles.
  • Ayae questions whether the transformation actually halves the angles, referencing the mapping e^{iθ} to e^{2iθ}.
  • Another participant clarifies the direction of the mapping, asserting that a curve γ is mapped to {z² | z ∈ γ}, emphasizing the effect of squaring on the angles of rays in the complex plane.

Areas of Agreement / Disagreement

Participants generally agree on the relationship between holomorphic functions and conformality, but there is disagreement regarding the specifics of angle transformations at stationary points, particularly whether angles are halved or doubled.

Contextual Notes

There are unresolved aspects regarding the precise nature of angle transformations and the implications of higher order terms in the context of conformal mappings.

ayae
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Recently I have been self teaching myself complex analysis.

I am interested in the conformal mapping property of holomorphic functions and why and how it breaks down at stationary points.

Could anyone suggest further reading for this or shed some light on the subject.

Many thanks,
Ayae
 
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An intuitive explanation for why holomorphic implies conformal can be seen from the power series expansion of a function.

A complex function, differentiable at 0 can be expressed as a power series in some finite circle around the origin: [itex]f(z)=f(0)+f'(0)z+f''(0)\frac{z^2}{2!}+\cdots[/itex]. Sufficiently near the origin, we can ignore the higher powers of z. So this is approximately just a (affine) linear function, as long as [itex]f'(0)\neq0[/itex]: a multiplication by a fixed complex number, which is just a rotation (by the argument) and dilation (by the modulus), followed by a translation. This is clearly conformal (and conversely every conformal transformation must locally look like this).

On the other hand, if f'(0) vanishes, the higher order terms are dominant so there is an additional power of z. So, for example, if the first nonvanishing derivative is the second, the function locally looks like [itex]z\mapsto z^2[/itex] (followed by rotation, dilation & translation). You just have to look at the polar form to see that this doubles angles at the origin so it isn't conformal.

Locally, any complex differentiable function looks like a power, so to understand the local behaviour you need only understand z, z2, z3 etc. This is all just heuristic, but hopefully it will help to understand why it works.
 
Thanks that really made sense. :approve:

henry_m said:
You just have to look at the polar form to see that this doubles angles at the origin so it isn't conformal.
One thing; does it not half the angles?
[tex]e^{i\theta}\rightarrow e^{2i\theta}[/tex]

http://www.wolframalpha.com/input/?i={Re[%28x%2Biy%29]%3D0%2C+Im[%28x%2Biy%29]%3D0}
http://www.wolframalpha.com/input/?i={Re[%28x%2Biy%29^2]%3D0%2C+Im[%28x%2Biy%29^2]%3D0}
 
ayae said:
One thing; does it not half the angles?
[tex]e^{i\theta}\rightarrow e^{2i\theta}[/tex]
I think you've got the direction of the map the wrong way round; a curve [itex]\gamma[/itex] gets mapped to [itex]\{z^2|z\in \gamma\}[/itex], not [itex]\{z|z^2\in \gamma\}[/itex]. Think about where each of the points goes after the function is applied to it. For example, the ray [itex]iy[/itex] with [itex]y>0[/itex]; after getting squared each of the points ends up on the negative real axis, doubling the ray's angle with the positive real axis. Hope that makes sense.
 

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