Algebraic Geometry Jottings 18

Prev TOC Next

Up till now, I’ve been using power series to parametrize branches:

x(t) = a0+a1t+a2t2+ ⋯,      y(t) = b0+b1t+b2t2+ ⋯

If the branch passes through the origin, then a0=b0=0. In the last post, we established Facts 4 and 5, assuming that y(t)=t for all branches, so x(t) = a0+a1y+a2y2+ ⋯.

That special assumption doesn’t always hold. As a fairly simple example, take this blue circle tangent to the x-axis:


(Ignore the red and greeen lines for a moment.) Solving for x in terms of y, we get x=\pm\sqrt{y}\sqrt{4-y}. While \sqrt{4-y} can be expanded in a Taylor series about 0, \sqrt{y} cannot. It’s clear enough why we can’t express x as a power series in y near 0: the derivative dx/dy is infinite at y=0, wreaking havoc with the Taylor series.

In this case, we could switch the roles of x and y, getting the two branches y=2\pm\sqrt{4-x^2}, or near the origin, y=x^2/4+x^4/16+\cdots. But we’re not out of the woods yet. Say we wanted to verify Fact 5 for the intersections of the blue circle with the red line. At the other intersection, the circle is tangent to the green line, signifyiing an infinite dy/dx.

Even with a single curve, we could be in trouble. Consider the semicubical parabola y2=x3 (see Kendig Example 3.11, p.55):


We have either y=\pm\sqrt{x^3} or x=\omega^i\sqrt[3]{y^2} (with ω a primitive cube root of unity, i=0,1,2); neither is expressible as a power series about 0.

The solution: fractional power series, aka Puiseux series. For the circle, we have near 0


and for the semicubical parabola,

x=y^{3/2}    or    y=x^{2/3}.

Perhaps you have qualms about the ambiguity of n-th roots (as I did at first). In the next post, I will try to dispel these three ways: via extension fields, via Riemann surfaces, and via the theory of fractional power series. We’ll see that the ambiguity plays an essential role.

First let’s see how Facts 4 and 5 work out with this technique. Along the way, we’ll see how it squashes the “grade inflation bug” mentioned way back in post 3.

You can paper over the fractional exponents using a so-called uniformizing parameter t. For the circle, use t=y½, giving x=2t-t^3/4-t^5/16+\cdots. Chew on this for a moment, chomping down on the multiplicity of the intersection at O between the circle and the x-axis. That multiplicity is 2 because if (x_E(t),y_E(t)) is the branch (2t+\cdots,t^2) and F(x,y)=y is the x-axis, then F(t)=F(x_E(t),y_E(t))=t^2, and the equation F(t)=\epsilon has two solutions for \epsilon\approx 0. And furthermore, those two t‘s give two intersections because xE(t)≈2t. The “grade inflation bug” shows its feelers when we use y=t4 for the parametrization (for example).

If we stick with fractional exponents, the multiplicity calculation looks like this: the parametrization is

(x_E(t),y_E(t))= (2y^{1/2}+\cdots,y)

and F(x,y)=y. The equation F(x,y)=y=ϵ has only a single solution for any ϵ, but x≈½ has two possible values because of the ambiguity of the square root, when ϵ≠0. So we get two intersections when we perturb things slightly.

As an instructive comparison, let F(x,y)=y–x be the red diagonal line. Plugging in the parametrization now gives F(x,y)≈y–2y½. Before we had two values of x for one value of F. Now we have two values of x for two values of F (near but not at O), because both have y½ as their lowest power of y. One F for one x, multiplicity 1.

Let’s generalize. If E(x,y) is monic as a polynomial in x, then any branch crossing the x-axis has a parametrization

(x_E,y_E)= (a_ky^{k/d}+a_{k+1}y^{(k+1)/d}+\cdots,y)

with ak≠0 and all the exponents having the same denominator d (see Kendig §3.4, p.54). As usual, we care only about the lowest-order term, so assume that k and d are coprime—it doesn’t matter if higher-order exponents require a larger denominator. Clearly the lowest-order term of F(xE,yE) will have the form cy^{r/d}. Claim: the multiplicity of the intersection (between the branch of E and the curve F) is r. This is easiest to see when k=1. Introduce the parameter t=y1/d. For a given y≠0, there are d different values of t. Since x=a1t+a2t2+ ⋯, that means d different values of x for any y near but not equal to 0. Now, how many of these land on the level curve F(x,y)=ϵ? Since F(xE,yE)≈ctr, the answer is r: to the r different solutions to ctr=ϵ correspond r different values of x. Multiplicity r, in other words.

This is a good spot to discuss conjugate parametrizations (see Kendig p.55). The parameter t belongs to the family of d conjugate parameters t, ωt, …, ωd–1t, where ω is a primitive d-th root of unity. As t “fills out” a small disk |t|<δ in the complex plane, so do all of its conjugates (as Kendig puts it). Since y=td, all the conjugate values give the same y, but different x‘s. We get the same branch, in the sense of the totality of (x,y) values, but d different parametrizations of it.

It’s particularly easy to picture all this for the blue circle above, since d=2 and the conjugate values are ±t. Restricting attention to real values of t near 0, one parametrization traces a small arc of the circle near O from left to right, the other from right to left. For the level curves which are lines parallel to the x-axis, two values of t land on the curve; for the level curves which are lines parallel to the red line, only one (keeping t small).

We have to make almost no changes to this argument when k≠1, provided k is still coprime to d (as assumed). We still get d different values of x for the d values of t and that’s all we need. A little number theory furnishes the proof of this claim. Namely, the exponents of ω essentially belong to the ring ℤ/dℤ, and k is a unit in that ring: lk≡1 mod d for some l, since gcd(k,d)=1 implies lk+qd=1 for some l and q. That means that as j ranges from 0 to d-1, (ωjt)kkjtk takes on d different values. Incidentally, the need for k to be coprime to d prevents the grade inflation bug: replacing d with a multiple is forbidden.

Very good, we now understand multiplicity when using fractional power series. How about the proof of Fact 4? Once again we consider the formula

\text{res}_x(E,F) = a_m^n \prod_{i=1}^m F(u_i(y))    (2)

where we assume that the leading coefficient am is a constant, and the x-degree of E is m, of F is n. Key point: the ui(y)’s must include all the conjugate parametrizations of each branch. Otherwise we won’t get m of them! (See Kendig pp.55–56. We saw a similar situation in post 10 with the two-ellipse example: we had to include both positive and negative square roots in the factorizations.)

Among the E-branches crossing the x-axis, we might find all sorts of denominators d. (When d=1, we have the special case treated in the last post.) We need to show that an E-branch intersecting F with multiplicity r on the x-axis, contributes a factor of yr to the lowest-order term in eq.(2). Multiplicity r means that the lowest-order term of F(ui) looks like cyr/d. With all its d conjugates, we get a contribution of (yr/d)d. All’s right with the world!

Finally, Fact 5 follows from Fact 4 just as in the last post.

Prev TOC Next

Leave a comment

Filed under Algebraic Geometry

Leave a Reply

Fill in your details below or click an icon to log in: Logo

You are commenting using your account. Log Out /  Change )

Facebook photo

You are commenting using your Facebook account. Log Out /  Change )

Connecting to %s

This site uses Akismet to reduce spam. Learn how your comment data is processed.