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math121a-f23:september_11_monday

Holomorphic Function, Meromorphic Function

tl;dr

A function f:CC{}f: \C \to \C \cup \{\infty\} is holomorphic at z0z_0 if there exists ϵ>0\epsilon>0, and complex numbers a0,a1,a_0,a_1,\cdots that for all zz0<ϵ|z - z_0|<\epsilon, we can write f(z)=n=0an(zz0)n. f(z) = \sum_{n=0}^\infty a_n (z-z_0)^n.

A function f:CC{}f: \C \to \C \cup \{\infty\} is meromorphic at z0z_0 with order m1m \geq 1 pole, if there exists ϵ>0\epsilon>0, and complex numbers am,,a0,a1,a_{-m}, \cdots , a_0,a_1,\cdots that for all 0<zz0<ϵ0 < |z - z_0|<\epsilon, we can write f(z)=n=man(zz0)n. f(z) = \sum_{n=-m}^\infty a_n (z-z_0)^n.

Real function Differentiability

First, let's us recall some notion in real analysis. Given a function f:RRf: \R \to \R, we can talk about its derivative at a point x0Rx_0 \in \R. It is defined as f(x0)=limϵ0f(x0+ϵ)f(x0)ϵ. f'(x_0) = \lim_{\epsilon \to 0} \frac{f(x_0 + \epsilon) - f(x_0)} {\epsilon}. If the derivative f(x0)f'(x_0) exists, then we say the function ff is differentiable at x0x_0. For example, f(x)=xf(x) =|x| is not differentiable at x=0x=0. If the derivative f(x0)f'(x_0) exists for all x0Rx_0 \in \R, then we say ff is differentiable on R\R.

Ex 1 f(x)={xx02xx0 f(x) = \begin{cases} x & x \geq 0 \cr 2 x & x \leq 0 \end{cases} Is it differentiable at x=0x=0? Can you plot f(x)f'(x)?

Ex 2 f(x)={x2x02x2x0 f(x) = \begin{cases} x^2 & x \geq 0 \cr 2 x^2 & x \leq 0 \end{cases}

Is it differentiable at x=0x=0? Can you plot f(x)f'(x)? (this is an example, where the function f(x)f(x) is differentiable, but the derivative f(x)f'(x) is not continuous, hence we cannot define f(x)f^{“}(x) at x=0x=0, hence f(x)f(x) is not a smooth function on R\R).

Complex function Differentiability

On the face value, the definition for complex differentiability is just replacing the word 'real' by 'complex', in the above section.

Definition: we say f:CCf: \C \to \C is differentiable at z0Cz_0 \in \C, if f(z0)=limϵ0f(z0+ϵ)f(z0)ϵ exists. f'(z_0) = \lim_{\epsilon \to 0} \frac{f(z_0 + \epsilon) - f(z_0)} {\epsilon} \quad \text{ exists.}

Remark: Here ϵ\epsilon can go to 00 in different directions, we can let ϵ=reiθ\epsilon = r e^{i\theta} for fixed θ\theta and positive r0r \to 0. The condition that derivative exists really means no matter how ϵ\epsilon approach 00, the above limit exists.

Let's see some example.

  • f(z)=z3 f(z) = z^3 at z0z_0, what is f(z0)f'(z_0)?
  • f(z)=z2 f(z) = |z|^2 at z0=0z_0 = 0, at z0=1|z_0|=1. Does f(z0)f'(z_0) exist?

Definition: we say a subset ΩC\Omega \In \C is an 'open subset of C\C', or simply 'open', if for any point pΩp \in \Omega, we can enlarge it to a small ball Bϵ(p)ΩB_\epsilon(p) \In \Omega, where Bϵ(p)={zzp<ϵ}B_\epsilon(p) = \{ z \mid |z-p| < \epsilon \}.

Example: the strip Re(z)<1| Re(z) | < 1 is open; the line Rez=1Re z = 1 is not open.

Definition: We say a function f:ΩCf: \Omega \to \C is an analytic function (aka holomorphic) on Ω\Omega if for any pΩp \in \Omega, f(p)f'(p) exists.

Example:

  • f(z)=1/zf(z) = 1/z is holomorphic on Ω=C\{0}\Omega = \C \RM \{0\}.
  • f(z)=1/(z2+1)f(z) = 1/ (z^2+1) is holomorphic on Ω={zCz2+10}=C\{±i}\Omega = \{z \in \C \mid z^2 + 1 \neq 0 \} = \C \RM \{ \pm i \}.

Taylor expansion

Suppose f:ΩCf: \Omega \to \C is a holomorphic function on Ω\Omega.

Then the derivative f(p)f'(p) exists for every point pp in Ω\Omega by definition. Furthermore, f:ΩCf': \Omega \to \C itself is a holomorphic function (a non-trivial result, not true for real differentiable function). Hence, we can differentiate ff anytimes we want on Ω\Omega.

The Taylor expansion of ff centered at point pΩp \in \Omega is the following identity. If Br(p)ΩB_r(p) \In \Omega, then for any zBr(p)z \in B_r(p), we have f(z)=f(p)+f(p)(zp)+f(p)(zp)22!++f(n)(p)(zp)2n!+. f(z) = f(p) + f'(p) (z-p) + f”(p) \frac{ (z-p)^2}{2!} + \cdots + f^{(n)}(p) \frac{ (z-p)^2}{n!} + \cdots.

Point Singularity

Suppose f:C\{0}Cf: \C \RM \{0\} \to \C is holomorphic function, you cannot help but wonder, what goes wrong at 00? You might find

  • a removable singularity (i.e. a false alarm, ff is all good at z=0z=0)
  • a pole, znf(z)z^n f(z) is holomorphic
  • an essential singularity: anything else, like e1/ze^{1/z}, e1/z2e^{1/z^2}.

If you had a pole, we can apply that Taylor expansion formula (at z=0z=0) to znf(z)z^n f(z), then divide out by zz.

Exercises

Find the first two terms in these expansions.

1. Taylor expand (z+1)(z+2)(z+1)(z+2) around z=3z=3.

2. Laurent expand 1/[(z1)(z2)]1/[(z-1)(z-2)] around z=1z=1. And do it again, this time around z=2z=2.

2.5 (Optional) Laurent expand e1/z+ze^{1/z + z} around z=0z=0.

3. You may have heard about Cauchy Riemann equation: let f(z)f(z) be a C\C-valued function on C\C, and let z=x+iyz = x+iy, f=u+ivf = u+iv, then we can view u,vu,v as real valued functions depending on x,yx,y.

If ff is holomorphic, then we have u(x,y)x=v(x,y)y,v(x,y)x=u(x,y)y \frac{\d u(x,y)}{\d x} = \frac{\d v(x,y)}{\d y}, \quad \frac{\d v(x,y)}{\d x} = - \frac{\d u(x,y)}{\d y}

Your task: either prove this in general if you feel strong, or verify that this is true for your favorite holomorphic function (don't choose ff to be a constant, too boring)

math121a-f23/september_11_monday.txt · Last modified: 2023/09/15 21:41 by pzhou