Section 3.6

Vector fields in the plane

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Problem 3.6.1

Give the details for the claim that the degree of vmx,rvm_{x,r} does not depend on the choice of radius rr as long as we are inside a disk where vv only vanishes at xx.

Setup: a vector field on X⊂R2X \subset \mathbb {R}^{2} is a continuous function v:X→R2v : X \rightarrow \mathbb {R}^{2}. For a circle of radius rr about a point xx, let mx,r(z)=x+rzm_{x,r}(z) = x + rz, giving a map vmx,r:S1→R2vm_{x,r} : S^1 \rightarrow \mathbb {R}^{2}; if vv does not vanish on this circle, deg⁡(vmx,r)\deg (vm_{x,r}) is defined as usual (via the normalized map z↦vmx,r(z)/∣vmx,r(z)∣z \mapsto vm_{x,r}(z)/\left|vm_{x,r}(z)\right| into S1S^1). A point xx where vv vanishes is called a singularity; it is isolated if there is a deleted neighborhood of xx where vv is nonzero. For an isolated singularity xx, the index i(x)i(x) is the degree of vmx,rvm_{x,r} for a small enough rr that the only zero inside the disk of radius rr about xx is xx itself.

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Remark.
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Use Proposition 3.5.10(3): if F:A(r1,r2)→R2∖{0}F : A(r_1, r_2) \rightarrow \mathbb {R}^{2} \setminus \left\{ 0\right\} is continuous on the closed annulus A(r1,r2)={z:r1≤∣z∣≤r2}A(r_1, r_2) = \left\{ z : r_1 \leq \left|z\right| \leq r_2\right\}, then deg⁡F∣r2S1=deg⁡F∣r1S1\deg F \vert r_2 S^1 = \deg F \vert r_1 S^1.

Problem 3.6.2

Give an explicit construction of the homotopy of vm2,1vm_{2,1} to zz described in the computation of the index of the vector field v(z)=z(z−2)v(z) = z(z-2) at its singularity 22.

Recall the analogous computation at the singularity 00: z−2z - 2 extends to a map of the unit disk into R2∖{0}\mathbb {R}^{2} \setminus \left\{ 0\right\}, so H(z,t)=tz−2H(z,t) = tz - 2 is a homotopy into C∖{0}\mathbb {C} \setminus \left\{ 0\right\} between z−2z-2 and the constant map −2-2; then V(z,t)=zH(z,t)V(z,t) = zH(z,t), normalized, gives a homotopy between v(z)v(z) and −z-z as maps S1→S1S^1 \rightarrow S^1, and −z-z is homotopic to zz via k(z,t)=eπitzk(z,t) = e^{\pi i t} z. For the singularity at 22, restrict to the circle of radius 11 about 22 and look at vm2,1(z)=(2+z)zvm_{2,1}(z) = (2+z)z; homotope the (2+z)(2+z) term to 22 to get a homotopy of this to 2z2z, which normalizes to a homotopy of vm2,1(z)vm_{2,1}(z) to zz.

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Problem 3.6.3

Each part of the figure below depicts the vector field on a circle about an isolated singularity. Determine the index of each of the singularities.

Vector fields for Exercise 3.6.3.Vector fields for Exercise 3.6.3.

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Problem 3.6.4

Give an example of a vector field in the plane which has two singularities of index 11 and one singularity of index −1-1.

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Remark.
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Start with a vector field with one singularity of index 11 and then introduce two new singularities that look like the canceling-singularity pair shown below (constantly (1,0)(1,0) outside an oblong region, with two singularities of index 11 and −1-1 inside it whose total index is 00).

Another example of canceling singularities.Another example of canceling singularities.

Problem 3.6.5

Show that f:S1→S1f : S^1 \rightarrow S^1, f(z)=cf(z) = c (a constant), is homotopic to g(z)=1g(z) = 1.

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Problem 3.6.6

Show that, if f:S1→C∖{0}f : S^1 \rightarrow \mathbb {C} \setminus \left\{ 0\right\} satisfies f(z)=f1(z)f2(z)f(z) = f_1(z) f_2(z) (complex multiplication of f1f_1 and f2f_2) and f2f_2 is homotopic to f3f_3, then ff is homotopic to g(z)=f1(z)f3(z)g(z) = f_1(z) f_3(z).

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Problem 3.6.7

Show that, if f(z):S1→C∖{0}f(z) : S^1 \rightarrow \mathbb {C} \setminus \left\{ 0\right\} extends over the unit disk to F:D2→C∖{0}F : D^2 \rightarrow \mathbb {C} \setminus \left\{ 0\right\}, then f(z)f(z) is homotopic to g(z)=1g(z) = 1.

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Remark.
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Use the map G:S1×I→D2G : S^1 \times I \rightarrow D^2, G(z,t)=tzG(z,t) = tz, composed with FF to get a homotopy to the constant map F(0)F(0). Then use path connectivity in C∖{0}\mathbb {C} \setminus \left\{ 0\right\} to move F(0)F(0) to 11.

Problem 3.6.8

Give an explicit homotopy between f(z)=2z−5f(z) = 2z - 5 and g(z)=1g(z) = 1 as maps from S1S^1 to C∖{0}\mathbb {C} \setminus \left\{ 0\right\}.

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Problem 3.6.9

Suppose v(z)=v1(z)v2(z)v(z) = v_1(z) v_2(z) (complex multiplication) is a vector field with an isolated singularity at xx. Suppose v1(x)=0v_1(x) = 0, v2(x)≠0v_2(x) \neq 0, and the only singularity of vv inside B(x,r)B(x,r) is at xx. Show that the index of vv at xx as computed on the circle of radius rr about xx is the same as the index of v1v_1 as computed on the same circle.

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Problem 3.6.10

Suppose v(z)=(z−x1)⋯(z−xn)v(z) = (z-x_1) \cdots (z-x_n) is given as a factored polynomial. Show that vv has isolated singularities x1,…,xnx_1, \ldots , x_n and that each has index 11, so the index of the vector field is nn.

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Remark.
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Use the preceding exercise.

Problem 3.6.11

Verify that r:S1×I→D2r : S^1 \times I \rightarrow D^2, r(z,t)=tzr(z,t) = tz, is a quotient map, and that the induced map Kˉ′:D2→R2∖{0}\bar{K}' : D^2 \rightarrow \mathbb {R}^{2} \setminus \left\{ 0\right\} gives an extension of ff, in the context of the proof of the following lemma.

Lemma 3.6.1: Let f:S1→R2∖{0}f : S^1 \rightarrow \mathbb {R}^{2} \setminus \left\{ 0\right\} be a continuous map whose composition with u(z)=z/∣z∣u(z) = z/\left|z\right| has degree 00. Then ff extends to a continuous map from D2D^2 to R2∖{0}\mathbb {R}^{2} \setminus \left\{ 0\right\}.

In the proof, a homotopy K:I×I→(R2∖{0})K : I \times I \rightarrow (\mathbb {R}^{2} \setminus \left\{ 0\right\} ) between fpfp (where p(t)=e2πitp(t) = e^{2\pi i t}) and a constant map induces, since S1S^1 is a quotient of II via pp, a homotopy Kˉ:S1×I→R2∖{0}\bar{K} : S^1 \times I \rightarrow \mathbb {R}^{2} \setminus \left\{ 0\right\} with Kˉ(z,1)=f(z)\bar{K}(z,1) = f(z).

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Problem 3.6.12

Verify the claim made in the proof of the following proposition, for the base case k=1k=1: that the degree of vmx,rvm_{x,r} is the same as the degree of vmz1,r1vm_{z_1, r_1}, using a homotopy between the map mx,rm_{x,r} and the map mz1,r1m_{z_1, r_1} onto a small circle around the singularity z1z_1.

Proposition 3.6.2: Suppose vv is a vector field defined on the disk B(x,r)B(x,r) centered at xx which has isolated singularities at z1,…,zkz_1, \ldots , z_k. The degree of the map vmx,rvm_{x,r} is the sum of the indices of the singularities; that is, the index of the vector field may be computed by computing the degree using the vector field on the boundary circle.

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