JC2Exploring the plane Jacobian conjecture

Why adjoining a cube root can simplify a problem

At partial degrees six and nine the leading coefficients are a square and a cube of the same polynomial, and one cube root makes both of them one. The symmetry that comes with it grades every remaining equation.


Enlarging the field you work over looks like the wrong direction. You wanted to solve a problem over k(x)k(x), and now you have a bigger object with more elements in it. But an extension comes with a symmetry group, and a symmetry group sorts things. Sometimes the sorting is worth more than the simplicity you gave up.

Here is a case where the trade is obviously good.

Two leading coefficients, one root

The setting is a pair p,qk[x][y]p, q \in k[x][y] of outer degrees six and nine in yy, with a nonzero constant Keller bracket, and with leading coefficients that are not independent:

p=H2y6+,q=H3y9+p = H^{2}y^{6} + \cdots, \qquad q = H^{3}y^{9} + \cdots

for a single HH. The exponents are the thing to notice. Six and nine are both multiples of three, and the leading coefficients are the square and the cube of the same HH. Write

t=H1/3.t = H^{1/3} .

Then t6=H2t^{6} = H^{2} and t9=H3t^{9} = H^{3}, so in the variable z=tyz = t\,y both leading terms become z6z^{6} and z9z^{9}. One substitution makes both polynomials monic at once. That is the whole reason to adjoin the root: not to make the field bigger, but to make the two leading coefficients disappear together.

What you get in exchange

If HH is a cube in k(x)k(x) then tt was already there and nothing happened. The interesting case is when HH is a noncube. Then y3Hy^3 - H is irreducible, k(x)(t)k(x)(t) is a degree-three extension, and it is cyclic: the map

σ:tωt,ω3=1, ω1,\sigma : t \longmapsto \omega t, \qquad \omega^{3}=1,\ \omega \neq 1,

generates its automorphism group. Applying σ\sigma permutes the three cube roots t,ωt,ω2tt, \omega t, \omega^{2}t cyclically and fixes everything in k(x)k(x).

That gives a grading. Every element of the extension splits into three pieces according to how σ\sigma scales it: weight 00 for the pieces σ\sigma fixes, weight 11 for those it multiplies by ω\omega, weight 22 for ω2\omega^{2}. The weight-00 part is exactly k(x)k(x).

Figure 1

Left: the deck map rotates the three cube roots of HH into one another and fixes the base field. Right: it therefore sorts powers of tt into three weights. The weight-zero column is just 1,H,H21, H, H^{2}, which is to say the part that was in k(x)k(x) all along.

The grading is what does the work. An identity that has to hold over k(x)k(x) must hold weight by weight, so one equation in the extension becomes three separate equations, each shorter than the original. Better still, any expression built to be σ\sigma-invariant is automatically an expression in HH, with the cube root gone. The extension is scaffolding: you put it up, use the symmetry to organize the equations, and take it down again.

Alignment

The first place this pays is the leading Keller row. Cleared of denominators it says that a particular combination is constant under differentiation, and it is a weight-one quantity. A weight-one quantity that has to be fixed by σ\sigma has to be zero, because σ\sigma multiplies it by ω1\omega \neq 1. So the nontrivial cubic action forces that discriminator to vanish, which pins down a relation among the coefficients before any elimination starts. The campaign calls this alignment: the symmetry aligns the two polynomials with each other at no cost.

From there the argument depresses both polynomials simultaneously, integrates the eight high bracket rows into a normal form with five coefficients and one extra parameter, and then extracts the four lower rows. The invariant part splits into two sheets, and the remaining work is to rule each one out.

The statement

Noncube exclusion at partial degrees (6,9)(6,9). Let p,qk[x][y]p, q \in k[x][y] have outer degrees six and nine, leading coefficients H2H^{2} and H3H^{3}, and nonzero constant Keller bracket. If 3degH3 \mid \deg H, then HH cannot be a noncube.

It is formalized in Lean 4. The statement is worth reading carefully for what it does not contain: no preselected cubic extension, no affine normalization, no coefficient weights, no constant-field hypothesis, and no rational numerator and denominator presentation. All of that is constructed inside the proof from the literal polynomial hypotheses. That matters, because a statement that assumed the extension would be assuming the convenient half of the setup.

Three sheets have to be excluded to finish: a zero sheet, an elliptic sheet, and a shifted Davenport–Stothers sheet. They are excluded separately, and the third is the one that needs real work.

Scope

This is the noncube branch and nothing else. It does not prove the cube branch, where HH is a cube and the extension above is trivial, so the entire grading argument is unavailable and a different mechanism is needed. It does not cover all of (6,9)(6,9). It does not reach maximum partial degree eleven. It does not prove the plane Jacobian conjecture.

Saying which half is done is the point. The noncube case is the one where the symmetry exists, which is exactly why it fell first. The cube case is harder for a reason that the proof above makes clear rather than hides: there is no deck action to grade by.

A question to take away

The grading came free because HH was not a cube. When HH is a cube, k(x)(H1/3)=k(x)k(x)(H^{1/3}) = k(x) and there is no symmetry to exploit.

Is there a substitute? One direction worth trying is a different root: at partial degrees six and nine the exponents are divisible by three, but they are also even and odd respectively, so a square root behaves differently on the two polynomials. Another is to look for a grading that is not Galois at all, coming from a filtration rather than a group action. A mechanism that organizes the cube branch as cheaply as the deck action organizes the noncube branch would close the gap that this result leaves open, and it would probably be reusable well beyond (6,9)(6,9).