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Math416Complex Variables (Lecture 24)

Math416 Lecture 24

Continue on Generalized Cauchy’s Theorem

Homotopy

A homotopy between two curves γ0,γ1:[0,1]C\gamma_0, \gamma_1 : [0, 1] \to \mathbb{C} is a continuous map H:[0,1]×[0,1]CH : [0, 1] \times [0, 1] \to \mathbb{C} such that H(z,0)=γ0(z)H(z, 0) = \gamma_0(z) and H(z,1)=γ1(z)H(z, 1) = \gamma_1(z) for all z[0,1]z \in [0, 1].

Lemma:

Let Ω\Omega be open in C\mathbb{C}, Let γ0,γ1\gamma_0, \gamma_1 be closed contour, homotopic in Ω\Omega. Then indγ0(z)=indγ1(z)\operatorname{ind}_{\gamma_0} (z) = \operatorname{ind}_{\gamma_1} (z) for all zΩz \in \Omega.

Proof:

Let H(s,t)H(s,t) be a homotopy between γ0\gamma_0 and γ1\gamma_1. Let z0CΩz_0\in \mathbb{C} \setminus \Omega.

Defined ϕ:[0,1]×[0,1]C{0}\phi:[0,1]\times[0,1]\to \mathbb{C}\setminus \{0\}, ϕ(s,t)=H(s,t)z0\phi(s,t)=H(s,t)-z_0.

By Technical Lemma , \exists continuous ψ:[0,1]×[0,1]C\psi:[0,1]\times[0,1]\to \mathbb{C} such that eψ=ϕe^{\psi}=\phi.

For each tt, γt(s)=H(s,t)\gamma_t(s)=H(s,t) is a closed curve.

indγt(z0)=12πi[ψ(1,t)ψ(0,t)]\operatorname{ind}_{\gamma_t}(z_0)=\frac{1}{2\pi i}\left[\psi(1,t)-\psi(0,t)\right].

This is continuous (in tt), integer valued, thus constant.

QED

Theorem 9.14 Homotopy version of Cauchy’s Theorem

Let Ω\Omega be open, γ0,γ1\gamma_0, \gamma_1 be two piecewise continuous curves in Ω\Omega that are homotopic.

Then γ0f(z)dz=γ1f(z)dz\int_{\gamma_0} f(z) \, dz = \int_{\gamma_1} f(z) \, dz for all fO(Ω)f\in O(\Omega).

Proof:

Γ=γ0γ1\Gamma=\gamma_0-\gamma_1, then indΓ(z)=0\operatorname{ind}_{\Gamma}(z)=0 for all zCΩz\in \mathbb{C}\setminus \Omega.

QED

Corollary of Theorem 9.14

If γ0\gamma_0 is null-homotopic in Ω\Omega (i.e. γ0\gamma_0 is homotopic to a point), then γ0f(z)dz=0\int_{\gamma_0} f(z) \, dz = 0 for all fO(Ω)f\in O(\Omega).

Chapter 10: Further development of Complex Function Theory

Simple connectedness

Definition (non-standard) simply connected

Let Ω\Omega be a domain in C\mathbb{C}. We say Ω\Omega is simply connected if CΩ\overline{\mathbb{C}}\setminus \Omega is connected. (C=C{})\overline{\mathbb{C}}=\mathbb{C}\cup \{\infty\})

Example:

disk is simply connected.

annulus is not simply connected.

C\mathbb{C} is simply connected.

Any convex domain is simply connected.

Standard definition: Ω\Omega is simply connected if every closed curve in Ω\Omega is null-homotopic in Ω\Omega.

Theorem of equivalent definition of simply connected

For open connected subsets of C\mathbb{C}, the standard definition and the non-standard definition are equivalent.

Proved end of book.

Proposition for simply connected domain

Ω\Omega is simply connected     \iff every contour in Ω\Omega has winding number 00 about every point in CΩ\mathbb{C}\setminus \Omega.

Proof:

If Ω\Omega is simply connected, let γ\gamma be a curve in Ω\Omega, then indγ(z)=0\operatorname{ind}_{\gamma}(z)=0 for all zz in the unbounded component of CΩ\overline{\mathbb{C}}\setminus \Omega. This contains all of CΩ\mathbb{C}\setminus \Omega.

Conversely, assume Ω\Omega is not simply connected, then KL=CΩ\exists K\cup L=\overline{\mathbb{C}}\setminus \Omega, where KK and LL are disjoint closed, without loss of generality, assume L\infty\in L.

Let H=ΩK=CLH=\Omega\cup K=\mathbb{C}\setminus L.

HH is open, KK is compact subset of HH, so by Separation Lemma , γHK=Ω\exists \gamma\in H\setminus K=\Omega such that Kint(γ)K\subset \operatorname{int}(\gamma).

Theorem 10.3 Cauchy’s Theorem for simply connected domain

corollary of Proposition for simply connected domain

Let Ω\Omega be a simply connected domain, let γ\gamma be a closed curve in Ω\Omega. Then γf(z)dz=0\int_{\gamma} f(z) \, dz = 0 for all fO(Ω)f\in O(\Omega).

Proof:

Know that is true if indγ(z)=0\operatorname{ind}_{\gamma}(z)=0 for all zCΩz\in \mathbb{C}\setminus \Omega.

By Proposition, Ω\Omega is simply connected     \iff every closed curve in Ω\Omega has winding number 00 about every point in CΩ\mathbb{C}\setminus \Omega.

So the result is true.

QED

Theorem 10.4-6

The following condition are equivalent:

  1. Ω\Omega is simply connected.
  2. every holomorphic function on Ω\Omega has a primitive gg, i.e. g(z)=f(z)g'(z)=f(z) for all zΩz\in \Omega.
  3. every non-vanishing holomorphic function on Ω\Omega has a holomorphic logarithm.
  4. every harmonic function on Ω\Omega has a harmonic conjugate.

Proof:

(1)    (2)(1)\iff (2):

First we show (1)    (2)(1)\implies (2).

Assume Ω\Omega is simply connected.

Define g(z)=z0zf(w)dwg(z)=\int_{z_0}^{z} f(w) \, dw for z0Ωz_0\in \Omega fixed. Then by Cauchy’s Theorem, this definition does not depend on the path.

g(z+h)g(z)h=1h[zz+hf(w)dw]\frac{g(z+h)-g(z)}{h}=\frac{1}{h}\left[\int_{z}^{z+h} f(w) \, dw\right]

1h[zz+hf(w)dw]f(z)\frac{1}{h}\left[\int_{z}^{z+h} f(w) \, dw\right]\to f(z) as h0h\to 0.

So on [z,z+h]Ω[z,z+h]\subset \Omega, if f(w)f(z)<ϵ|f(w)-f(z)|<\epsilon, then g(z+h)g(z)hhf(z)<hϵ|\frac{g(z+h)-g(z)}{h}-hf(z)|<h\epsilon.

To show (2)    (1)(2)\implies (1), we prove ¬(1)    ¬(2)\neg (1)\implies \neg (2).

(1)    (3)(1)\iff (3):

If Ω\Omega is not simply connected, there is some closed curve γ\gamma and some z0nΩz_0\not in \Omega such that indγ(z0)0\operatorname{ind}_{\gamma}(z_0)\neq 0.

SO γ1zz0dz0\int_{\gamma} \frac{1}{z-z_0} \, dz\neq 0.

So 1zz0\frac{1}{z-z_0} does not have a primitive on Ω\Omega. 1zz0\frac{1}{z-z_0} have no logarithm on Ω\Omega.

This shows (3)    (1)(3)\implies (1).

Suppose Ω\Omega is simply connected.fO(Ω)f\in O(\Omega) and ff is non-vanishing. We want to show that ff has a logarithm on Ω\Omega.

Let z0Ωz_0\in \Omega be fixed. And alogf(z0)a\in \log f(z_0).

f(z)f(z)=g\frac{f'(z)}{f(z)}=g' Since gO(Ω)g\in O(\Omega), wecanassumewe can assume g(z_0)=a$.

g(z)=a+z0zg(w)dwg(z)=a+\int_{z_0}^{z} g'(w) \, dw

So

(feg)=feg+fegg=f(eg)=0(fe^{-g})'=f'e^g+fe^g g'=f(e^g)'=0

So feg=cfe^{-g}=c for some cCc\in \mathbb{C}.

So f=cegf=ce^g

QED

Continue on Residue Theorem on Thursday.

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