What is the Average Value of |dφ/dz|^2 over the Open Unit Disk?

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  • Thread starter Euge
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In summary, The average value of |dφ/dz|^2 over the open unit disk is an important concept in complex analysis, used to understand the behavior of a function on the disk and calculate its maximum and minimum values. To calculate it, we find the value of |dφ/dz|^2 at every point on the disk and take the integral over the disk's area. This value can be affected by the complexity and location of the function as well as any singularities or critical points on the disk. In real-world applications, it is used in image processing, signal analysis, fluid dynamics, and calculating the average rate of change in a system.
  • #1
Euge
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Here is this week's POTW:

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Suppose $a$ is a fixed complex number in the open unit disk $\Bbb D$. Consider the holomorphic mapping $\phi : \Bbb D \to \Bbb D$ given by $\phi(z) := (z - a)/(1 - \bar{a}z)$. Find, with proof, the average value of $\left\lvert\frac{d\phi}{dz}\right\rvert^2$ over $\Bbb D$, i.e., the integral $$\frac{1}{\pi}\iint_{\Bbb D} |\phi'(x + yi)|^2\, dx\, dy$$-----

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  • #2
I'm giving another week for members to solve this POTW. As a hint, consider writing the integral in polar coordinates, and note that the integrand can be written as an expression of the Poisson kernel.
 
  • #3
This week's problem was solved correctly by Opalg. You can read his solution below.
By the quotient rule, $\phi'(z) = \dfrac{1-\bar{a}z + \bar{a}(z-a)}{(1-\bar{a}z)^2} = \dfrac{1 - \bar{a}a}{(1-\bar{a}z)^2}$, and therefore $$|\phi'(z)|^2 = \phi'(z)\overline{\phi'(z)} = \frac{(1 - \bar{a}a)^2}{(1-\bar{a}z)^2(1-a\bar{z})^2} = \frac{(1 - \bar{a}a)^2}{(1-2\text{re}(\bar{a}z) + \bar{a}a\bar{z}z)^2}.$$ So we want to evaluate \(\displaystyle \frac1\pi \iint_{\Bbb D}\frac{(1 - \bar{a}a)^2}{(1-2\text{re}(\bar{a}z) + \bar{a}a\bar{z}z)^2}\,dA\), where $A$ denotes area measure. The substitution $z\mapsto e^{i\arg a}z$ leaves the integral unchanged (it just represents a rotation of the disc, which preserves the measure), and has the effect of replacing $a$ by $|a|$. For the rest of the proof I will write $a$ instead of $|a|$, so that $a$ is real, positive, and less than $1$.

Next, write the integral on terms of polar coordinates as $$ \frac{(1 - a^2)^2}\pi \iint_{\Bbb D}\frac{1}{(1-2a\,\text{re}(z) + a^2\bar{z}z)^2}\,dA = \frac{(1 - a^2)^2}\pi \int_0^1\int_0^{2\pi}\frac{1}{(1-2ar\cos\theta + a^2r^2)^2}\,r\,d\theta \,dr.$$ Taking the theta integral first, substitute $w = e^{i\theta}$ to get $$ \begin{aligned}\int_0^{2\pi}\frac{1}{(1-2ar\cos\theta + a^2r^2)^2}\,d\theta &= \oint_{\partial\Bbb D}\frac1{\bigl((1+a^2r^2) - ar(w+w^{-1})\bigr)^2}\frac{dw}{iw} \\ &= \oint_{\partial\Bbb D}\frac{-iw}{(arw^2 - (1+a^2r^2)w + ar)^2}dw \\ &= \oint_{\partial\Bbb D}\frac{-iw}{a^2r^2(w - ar)^2\bigl(w - \frac1{ar}\bigr)^2}dw. \end{aligned} $$ By the Cauchy Integral Formula (and the fact that $ar$ lies inside $\Bbb D$), that last integral is equal to $$ \begin{aligned}\frac{2\pi i}{a^2r^2}\frac d{dw}\biggl(\frac{-iw}{(w - \frac1{ar})^2}\biggr)\bigg|_{w=ar} &= \frac{2\pi}{a^2r^2}\frac{(w - \frac1{ar})^2 - 2ar(w - \frac1{ar})}{(w - \frac1{ar})^4}\bigg|_{w=ar} \\ &= \frac{2\pi}{a^2r^2}\frac{ar - \frac1{ar} - 2ar}{(ar - \frac1{ar})^3} \\ &= \frac{2\pi(1 + a^2r^2)}{(1 - a^2r^2)^3}.\end{aligned}$$ Now plug that into the $r$-integral and then make the substitution $s = a^2r^2$, to get $$ \begin{aligned} \frac1\pi \iint_{\Bbb D}\frac{(1 - \bar{a}a)^2}{(1-2\text{re}(\bar{a}z) + \bar{a}a\bar{z}z)^2}\,dA &= \frac{(1 - a^2)^2}\pi \int_0^1\frac{2\pi r(1+a^2r^2)}{(1 - a^2r^2)^3}dr \\ &= \frac{(1 - a^2)^2}{a^2}\int_0^{a^2}\frac{1+s}{(1-s)^3}ds \\ &= \frac{(1 - a^2)^2}{a^2}\int_0^{a^2}\biggl(\frac2{(1-s)^3} - \frac1{(1-s)^2} \biggr)ds \\ &= \frac{(1 - a^2)^2}{a^2}\biggl[\frac1{(1-s)^2} - \frac1{1-s}\biggr]_0^{a^2} \\ &= \frac{(1 - a^2)^2}{a^2}\frac{a^2}{(1 - a^2)^2} \\ &= \large 1 \quad! \end{aligned}$$

Edit. Euge has pointed out that my solution does not work when $a=0$. To deal with that case, note that the function then becomes $\phi(z) = z$. So $\phi'(z)$ is the constant $1$, and the average value of its square over $\Bbb D$ is also $1$. Thus the result \(\displaystyle \frac{1}{\pi}\iint_{\Bbb D} |\phi'(x + yi)|^2\, dx\, dy = 1\) still holds in that case.
 

What is the Average Value of |dφ/dz|^2 over the Open Unit Disk?

The average value of |dφ/dz|^2 over the open unit disk is a measure of the average rate of change of the angle of a function as it moves along the disk. It is an important concept in complex analysis and is often used to calculate various properties of functions.

Why is the Average Value of |dφ/dz|^2 over the Open Unit Disk important?

The average value of |dφ/dz|^2 over the open unit disk is important because it allows us to understand the behavior of a function on the disk as a whole. It can also be used to calculate the maximum and minimum values of a function on the disk.

How do you calculate the Average Value of |dφ/dz|^2 over the Open Unit Disk?

To calculate the average value of |dφ/dz|^2 over the open unit disk, we first need to find the value of |dφ/dz|^2 at every point on the disk. Then, we take the integral of these values over the disk and divide by the area of the disk. This will give us the average value.

What factors can affect the Average Value of |dφ/dz|^2 over the Open Unit Disk?

The average value of |dφ/dz|^2 over the open unit disk can be affected by the complexity of the function, the location of the disk, and the presence of singularities or critical points on the disk. These factors can change the rate of change of the function and therefore impact the average value.

How is the Average Value of |dφ/dz|^2 over the Open Unit Disk used in real-world applications?

The concept of average value of |dφ/dz|^2 over the open unit disk is used in various real-world applications such as image processing, signal analysis, and fluid dynamics. It can also be used to calculate the average rate of change of physical quantities in different areas of a system.

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