Fundamental Theorem of Algebra
Theorem of the week
This week's theorem of the week is the fundamental theorem of algebra, and the picture is the proof!Theorem
Every non degree-zero polynomial p(z) = a_nz^n + ...+ a_1z + a_0 has a root in \mathbb{C}.Picture proof
To see how the picture proves this, write z as Re^{i\theta}, then for all kz^k = R^ke^{k i \theta}
So for sufficiently large R the a_nz^n term dwarfs all the others and so the image of \{z\in\mathbb{C}: \lvert z \rvert = R\} must go around the origin n times, like the rubber band in the photo. But when R= 0 the image is just \{a_0\} which goes around the origin zero times. So, for some 0 < r < R the image of \{z\in\mathbb{C}: \lvert z \rvert = r\} must cross the origin. QED.
Less handwavy proof
In order to obtain a contradiction assume p(z) has no zeros. Then \frac{z^{n-1}}{p(z)} is everywhere differentiable, which in turn means that its closed loop integrals are zero^{(\dagger)}. So, letting \gamma_R be the circle \lvert z \rvert = R we have\begin{align} 0 &= \int_{\gamma_R}\frac{z^{n-1}}{p(z)}dz\\ &= \int_{0}^{2\pi}\frac{R^{n-1}e^{i(n-1)\theta}}{\sum_{k=0}^na_kR^ke^{ik\theta}}Rie^{i\theta}d\theta\\ &= i\int_{0}^{2\pi}\frac{R^ne^{in\theta}}{\sum_{k=0}^na_kR^ke^{ik\theta}}d\theta\\ &= i\int_{0}^{2\pi} \frac{d \theta}{\sum_{k=0}^na_kR^{k-n}e^{i(k-n)\theta}} \\ &\underset{R \to \infty}{\longrightarrow} \frac{2\pi i}{a_n} \\ \end{align}
which was the contradiction we were seeking.
Footnotes
(\dagger) Let's assume f(z) is differentiable in some open set containing \Omega and see if we can show that the closed loop integral around \Omega is zero. It's sufficient to show the real part is zero since if(z) is also differentiable. The following uses Gauss' divergence theorem, and the definition f(x+iy) = u(x,y)+iv(x,y):\begin{align} Re\left(\int_{\partial\Omega} f(z) dz\right) &= \int_{\partial\Omega} udx - vdy \\ &=\int_{\partial\Omega} (v,u) \cdot (-dy,dx) \\ &=\int_{\partial\Omega} (v,u) \cdot \hat{\textbf{n}} dl \\ &=\int_\Omega v_x + u_y dA \\ &= \int_\Omega Im\left(\frac{\partial f}{\partial x}\right) + Im\left(i\frac{\partial f}{\partial y}\right) dA \\ &= \int_\Omega Im\left(\frac{df}{dz}\right) + Im\left(-\frac{df}{dz}\right) dA \\ &= 0 \end{align}
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