Complex polynomial on the unit circle

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Homework Help Overview

The discussion revolves around a complex polynomial evaluated on the unit circle, specifically exploring the implications of the polynomial's coefficients and their relationship to the maximum modulus principle in complex analysis.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the representation of polynomial values on the unit circle and the significance of choosing specific angles to align complex phases. There is mention of using Cauchy's integral formula for derivatives and exploring alternative methods for separating coefficients. Some participants question the necessity of using established theorems versus personal approaches.

Discussion Status

Participants are actively engaging with the problem, sharing insights on the use of Cauchy's integral theorem and its implications for the coefficients of the polynomial. There is a recognition of the constraints imposed by analytic functions, and some productive guidance has been offered regarding the integration process and its effects on the coefficients.

Contextual Notes

There is a mention of the problem not being an assigned homework task but rather a means for one participant to refresh their complex analysis skills for an upcoming project. The discussion also reflects on the challenge of differentiating terms and the implications of upper limits on polynomial coefficients.

hilbert2
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Homework Statement
If ##p(z) = a_0 + a_1 z + \dots + a_n z^n##

and ##M = \max\left\{|p(z)|:|z|=1\right\}##

then show ##|a_k |\leq M## for all ##k=0,1,2,\dots ,n##
Relevant Equations
Complex number ##z## can be written as ##z= |z|e^{i\theta}## with ##\theta\in\mathbb{R}##.
So, the values of polynomial ##p## on the complex unit circle can be written as

##\displaystyle p(e^{i\theta}) = a_0 + a_1 e^{i\theta} + a_2 e^{2i\theta} + \dots + a_n e^{ni\theta}##. (*)

If I also write ##\displaystyle a_k = |a_k |e^{i\theta_k}##, then the complex phases of the RHS terms of equation (*) are

##\displaystyle\arg \left( a_k e^{ik\theta}\right) = k\theta + \theta_k##.

Now I should somehow choose ##\theta## so that those complex phases are as much on the same half-circle as possible, to make them not cancel out and show that having ##|a_k |> M## for some ##k## and ##M = \max\left\{|p(z)|:|z|=1\right\}## at the same time leads to contradiction.
 
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Can you use Cauchy's integral formula for the derivatives of ##p(z)##?
 
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Yes, that is probably the way how this is meant to be solved, I just thought it would be a good exercise to solve it some other way. This is not actual homework assigned for me, I just have to refresh my complex analysis skills because of the project I'm working on right now.
 
The problem is to separate a specific coefficient, which is best done by differentiation. I first thought about multiplying a factor ##|z|^k##, but then we are left with terms ##|z|^p## as well as ##|z|^{-q}## and we don't know whether ##|z| \to 0## or ##|z| \to \infty## is the key. Differentiation kills the lower terms.

If you do not want to use Cauchy, then - as ##p(z)## is smooth - the mean value theorem for ##p^{(k)}## could be an idea.
 
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If at all possible, you should use those powerful theorems rather than your own ingenuity. They show, and make use of, how constrained analytic functions really are.
 
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Ok, so the Cauchy integral theorem says

##\displaystyle p(0) = a_0 = \frac{1}{2\pi i}\oint_\gamma\frac{p(z)}{z}dz =\frac{1}{2\pi i} \int_{0}^{2\pi}\frac{p(\gamma (t))}{\gamma(t)}\gamma'(t)dt##

and

##\displaystyle p^{(k)}(0) = k!a_k = \frac{1}{2\pi i}\oint_\gamma\frac{p^{(k)}(z)}{z}dz = \frac{1}{2\pi i}\int_{0}^{2\pi}\frac{p^{(k)}(\gamma(t))}{\gamma(t)}\gamma'(t)dt##,

where the path ##\gamma (t)=e^{it}## for ##t\in[0,2\pi]##. This is the counterclockwise path on complex unit circle.

Writing the integral for the case of ##a_0##, I have

##\displaystyle a_0 = \frac{1}{2\pi i}\int_{0}^{2\pi}\frac{a_0 + a_1 e^{it} + a_2 e^{2it} + \dots + a_n e^{nit}}{e^{it}}\cdot (ie^{it}) dt \\ \displaystyle = \frac{1}{2\pi}\int_{0}^{2\pi}\left(a_0 + a_1 e^{it} + a_2 e^{2it} + \dots + a_n e^{nit}\right) dt##.

The reason why only ##a_0## is left after the last integration is that the ##2\pi##-periodic functions ##a_k e^{ikt}## have a zero integral over one period.

Also, if the integrand ##\left(a_0 + a_1 e^{it} + a_2 e^{2it} + \dots + a_n e^{nit}\right)## is smaller than some upper limit ##M>0## in absolute value for all ##t\in [0,2\pi]##, then the result of integration, ##a_0##, can't be greater than ##2\pi M## in absolute value either. So this is why an upper limit for ##|p(z)|## on path ##\gamma## also limits the coefficient ##a_0##.

Now I just have to do the same for derivatives of ##p(z)##... Thanks for the advice.
 
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The version for the other coefficients ##a_k## is

##\displaystyle a_k = \frac{p^{(k)}(0)}{k!} = \frac{1}{2\pi i}\oint_\gamma \frac{a_0 + a_1 z +\dots +a_n z^n}{z^{k+1}}dz = \\ \displaystyle\frac{1}{2\pi} \int_{0}^{2\pi}\left(a_0 e^{-ikt} + a_1 e^{-i(k-1)t} + \dots + a_n e^{-i(k-n)t}\right)dt \\ \displaystyle = \frac{1}{2\pi}\int_{0}^{2\pi}e^{-ikt}\left(a_0 + a_1 e^{it} + a_2 e^{2it} + \dots + a_n e^{int}\right)dt,##

where in the last integral, the modulus of factor ##e^{-ikt}## is ##1## and the modulus of ##(a_0 + a_1 e^{it} + \dots )## is less than or equal to the upper limit ##M## in the statement of the problem. Therefore, also ##a_k \leq M##. ##\square##

Edit: and only when ##a_k## is the only coefficient that differs from zero, there's no better upper limit...
 
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