Holomorphic functions at stationary points

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Holomorphic functions exhibit conformal mapping properties, which break down at stationary points where the derivative vanishes. Near such points, the function can be approximated by a power series, and if the first non-vanishing derivative is of order two, the mapping results in angle doubling rather than preserving angles, thus losing conformality. The discussion highlights that while a non-zero derivative leads to local affine transformations that are conformal, a zero derivative introduces higher-order terms that dominate the behavior. This distinction is crucial for understanding the local behavior of complex functions. The conversation emphasizes the importance of analyzing the polar form of functions to grasp these transformations.
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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: f(z)=f(0)+f'(0)z+f''(0)\frac{z^2}{2!}+\cdots. Sufficiently near the origin, we can ignore the higher powers of z. So this is approximately just a (affine) linear function, as long as f'(0)\neq0: 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 z\mapsto z^2 (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?
e^{i\theta}\rightarrow e^{2i\theta}

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?
e^{i\theta}\rightarrow e^{2i\theta}
I think you've got the direction of the map the wrong way round; a curve \gamma gets mapped to \{z^2|z\in \gamma\}, not \{z|z^2\in \gamma\}. Think about where each of the points goes after the function is applied to it. For example, the ray iy with y>0; 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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