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Erdős 699: finiteness on every fixed algebraic curve

P699 research · The endpoint divisibilities · The elliptic approach


Every fixed algebraic curve in the (n,j)(n,j)-plane contains only finitely many bad pairs with index three. The odd part of nn may vary without restriction. More generally, the result holds for the endpoint conditions together with a fixed finite set of allowed denominator primes for j/nj/n.

Finiteness for each fixed exponent hh was already known from 3u3<2h3u^3<2^h. The theorem here permits hh to grow without bound while fixing an arbitrary polynomial relation F(n,j)=0F(n,j)=0.

The proof uses Siegel's theorem to reduce to rational curves, polynomial abc to remove a common factor from the remaining parameterization, and the two-circle argument below to finish.

This is not global finiteness: an infinite set in the plane can meet every fixed curve only finitely often. It does mean that a global Zariski nondensity theorem would now imply finiteness of all bad cubic pairs, without first bounding the odd part of nn.

1. A polynomial rigidity lemma

Lemma. Let N(X)=aXdN(X)=aX^d, where a>0a>0 and d≥1d\ge1, and let J∈R[X]J\in\mathbb R[X] have degree at most dd. Suppose

N−1∣J(J−1),N−2∣J(J−1)(J−2).(1)N-1\mid J(J-1),\qquad N-2\mid J(J-1)(J-2).\tag{1}

Then

J∈{0,1,N,N−1,2N−2,2−N}.(2)J\in\{0,1,N,N-1,2N-2,2-N\}.\tag{2}

Proof. Write J(X)=∑i=0dbiXiJ(X)=\sum_{i=0}^d b_iX^i, and let ζ\zeta range over the ddth roots of unity. Set

R1=a−1/d,R2=(2/a)1/d.R_1=a^{-1/d},\qquad R_2=(2/a)^{1/d}.

For every ζ\zeta, the first divisibility says that J(R1ζ)∈{0,1}J(R_1\zeta)\in\{0,1\}, while the second says that J(R2ζ)∈{0,1,2}J(R_2\zeta)\in\{0,1,2\}. In particular both sets of values are real.

Since the bib_i are real, reality on a circle of radius RR gives

∑i=0dbiRiζi=∑i=0dbiRiζ−i.\sum_{i=0}^d b_iR^i\zeta^i =\sum_{i=0}^d b_iR^i\zeta^{-i}.

The characters 1,ζ,…,ζd−11,\zeta,\ldots,\zeta^{d-1} are linearly independent as functions on the ddth roots of unity. Comparing their coefficients gives

biRi=bd−iRd−i(1≤i≤d−1).(3)b_iR^i=b_{d-i}R^{d-i}\qquad(1\le i\le d-1).\tag{3}

Apply (3) at both radii. Since R2/R1=21/d≠1R_2/R_1=2^{1/d}\ne1, a nonzero bib_i requires i=d−ii=d-i. Thus

J(X)=λN(X)+μJ(X)=\lambda N(X)+\mu

unless dd is even, in which case there can also be a term bXd/2bX^{d/2}.

Suppose that this extra term is nonzero. On the first circle, its two values are

λ+μ±b/a.\lambda+\mu\pm b/\sqrt a.

They are distinct and both belong to {0,1}\{0,1\}, so their absolute difference is one. On the second circle the two values instead have absolute difference 2\sqrt2. This is impossible for two members of {0,1,2}\{0,1,2\}. Hence the extra term vanishes.

Finally λ+μ∈{0,1}\lambda+\mu\in\{0,1\} and 2λ+μ∈{0,1,2}2\lambda+\mu\in\{0,1,2\}. The six choices give exactly (2). □\square

In particular, no such polynomial family can satisfy 4≤J(X)<N(X)/24\le J(X)<N(X)/2 for arbitrarily large positive XX.

2. Polynomial abc removes the common factor

We use the following characteristic-zero form of Mason–Stothers: if nonzero pairwise coprime polynomials U,V,WU,V,W, not all constant, satisfy U+V=WU+V=W, then

max⁡(deg⁡U,deg⁡V,deg⁡W)≤deg⁡rad⁡(UVW)−1.(4)\max(\deg U,\deg V,\deg W) \le\deg\operatorname{rad}(UVW)-1.\tag{4}

Here rad⁡\operatorname{rad} retains each distinct irreducible factor once. For a short proof, the nonzero Wronskian U′V−UV′U'V-UV' is divisible by UVW/rad⁡(UVW)UVW/\operatorname{rad}(UVW): at a root of any of the three polynomials of multiplicity bb, it vanishes to order at least b−1b-1. Comparing degrees gives the bound for deg⁡W\deg W; permutation gives the other two. This is also the statement proved in Mathlib's Mason–Stothers theorem.

Lemma. Let

N=TrD,J=LD,r≥1,D,L∈Q[T]∖{0},L(0)≠0,deg⁡L≤r.N=T^rD,\qquad J=LD,\qquad r\ge1,\quad D,L\in\mathbb Q[T]\setminus\{0\},\quad L(0)\ne0,\quad\deg L\le r.

Suppose

A=3J(J−1)N−1,B=J(J−1)(J−2)(N−1)(N−2)(5)A=\frac{3J(J-1)}{N-1},\qquad B=\frac{J(J-1)(J-2)}{(N-1)(N-2)}\tag{5}

are polynomials, and 4≤J(T)<N(T)/24\le J(T)<N(T)/2 holds for an unbounded sequence of positive real TT. Then DD is constant. In fact these hypotheses are impossible, by the two-circle lemma.

Proof. Put S=TrS=T^r, e=deg⁡De=\deg D, and ℓ=deg⁡L\ell=\deg L. The physical inequalities give deg⁡(S−L)=r\deg(S-L)=r. Also JJ is nonconstant: otherwise the first quotient in (5) would force J∈{0,1}J\in\{0,1\}. Thus ℓ+e>0\ell+e>0.

Since gcd⁡(D,(N−1)(N−2))=1\gcd(D,(N-1)(N-2))=1 and D∣JD\mid J, (5) implies D∣A,BD\mid A,B. Consequently the normalized coefficient cubic

P(z)=B+(A−3B)z+(3J−2A+3B)z2+(N−3J+A−B)z3D(6)P(z)=\frac{B+(A-3B)z+(3J-2A+3B)z^2 +(N-3J+A-B)z^3}{D}\tag{6}

belongs to Q[T,z]\mathbb Q[T,z] and satisfies P(1)=SP(1)=S. Its coefficients equal those of

6D(N−1)(N−2)∑i=03(J3−i)(N−Ji)zi.\frac{6}{D(N-1)(N-2)} \sum_{i=0}^3\binom J{3-i}\binom{N-J}{i}z^i.

The two polynomials

k=3L(S−L)N−1,q=L(S−L)(S−2L)(N−1)(N−2)(7)k=\frac{3L(S-L)}{N-1},\qquad q=\frac{L(S-L)(S-2L)}{(N-1)(N-2)}\tag{7}

are also in Q[T]\mathbb Q[T]. Indeed, modulo N−1N-1 the product J(N−J)J(N-J) is −J(J−1)-J(J-1), and modulo N−2N-2 the product J(N−J)(N−2J)J(N-J)(N-2J) is 2J(J−1)(J−2)2J(J-1)(J-2). The divisibilities in (5), and coprimality with DD, give (7). Neither polynomial is zero; for qq this also follows from N−2J>0N-2J>0 along the given sequence.

Write κ=deg⁡k\kappa=\deg k and λ=deg⁡q\lambda=\deg q. Then

κ=ℓ−e,λ≤ℓ−2e.(8)\kappa=\ell-e,\qquad \lambda\le\ell-2e.\tag{8}

The inequality for λ\lambda also handles cancellation in the leading term of S−2LS-2L when J/NJ/N tends to 1/21/2. The cubic discriminant identity gives

k3−27q2=T2rH,H=Disc⁡zP4∈Q[T].(9)k^3-27q^2=T^{2r}H,\qquad H=\frac{\operatorname{Disc}_z P}{4}\in\mathbb Q[T].\tag{9}

It can be checked directly from (6) and (7); equivalently,

H=27L2(S−L)2(DL−1)(D(S−L)−1)(N−1)3(N−2)2.H=\frac{27L^2(S-L)^2(DL-1)(D(S-L)-1)} {(N-1)^3(N-2)^2}.

The displayed expression is positive on the given physical sequence, so H≠0H\ne0. Moreover, k(0)=3L(0)2k(0)=3L(0)^2 and q(0)=L(0)3q(0)=L(0)^3, so T∤kqT\nmid kq.

Let G=gcd⁡(k3,q2)G=\gcd(k^3,q^2). Since T∤GT\nmid G, (9) implies G∣HG\mid H. Apply (4) to the pairwise coprime polynomials

k3G,−27q2G,T2rHG.\frac{k^3}{G},\qquad -\frac{27q^2}{G},\qquad T^{2r}\frac HG.

They are not all constant, since the last has a zero at zero. Their distinct roots lie among the roots of kk, qq, TT, and H/GH/G. Apply (4) to the degree of the third polynomial. It gives

2r+deg⁡(H/G)≤κ+λ+deg⁡(H/G).2r+\deg(H/G)\le\kappa+\lambda+\deg(H/G).

Cancel the common term and use (8):

2r≤κ+λ≤2ℓ−3e≤2r−3e.2r\le\kappa+\lambda\le2\ell-3e\le2r-3e.

Therefore e=0e=0, as required. Now N=aTrN=aT^r with a>0a>0, and the two-circle lemma applied to (5) excludes the physical inequalities. □\square

3. Finiteness on every fixed algebraic curve

Theorem. Fix a finite set S\mathcal S of rational primes and a nonzero polynomial F∈Q[n,j]F\in\mathbb Q[n,j]. There are only finitely many integer pairs (n,j)(n,j) satisfying

4≤j<n/2,F(n,j)=0,jn,3j(j−1)n−1,j(j−1)(j−2)(n−1)(n−2) ∈Z[S−1].(10)\begin{gathered} 4\le j<n/2,\qquad F(n,j)=0,\\ \frac jn,\quad \frac{3j(j-1)}{n-1},\quad \frac{j(j-1)(j-2)}{(n-1)(n-2)} \ \in\mathbb Z[\mathcal S^{-1}]. \end{gathered}\tag{10}

The last two quantities may in particular be integers. Every bad pair with index three satisfies (10) with S={2,3}\mathcal S=\{2,3\}. Indeed the endpoint conditions make the last two quantities integers, and 3j/u∈Z3j/u\in\mathbb Z for n=2hun=2^hu gives j/n∈13Z[1/2]j/n\in\tfrac13\mathbb Z[1/2].

Proof. Suppose infinitely many pairs satisfy (10). Choose an irreducible component of F=0F=0 containing infinitely many of them. It is geometrically irreducible: otherwise its rational points lie in finite intersections of distinct geometric conjugate components. The function nn is nonconstant, since each fixed row has only finitely many admissible columns.

Take the affine graph of the five rational functions

n,j,j/n,A=3j(j−1)n−1,B=j(j−1)(j−2)(n−1)(n−2).n,\quad j,\quad j/n,\quad A=\frac{3j(j-1)}{n-1},\quad B=\frac{j(j-1)(j-2)}{(n-1)(n-2)}.

It has infinitely many S\mathcal S-integral points. Siegel's theorem therefore says that its smooth projective model has genus zero and at most two geometric points at infinity, meaning the union of poles of these five functions. The precise SS-integral statement is recalled in Corvaja–Zannier's primary abstract. The model has rational points and hence is P1\mathbb P^1 over Q\mathbb Q.

First, j/nj/n cannot be constant. Otherwise j=θnj=\theta n for some 0<θ<1/20<\theta<1/2. The function AA has poles over n=1n=1, and BB has poles over n=2n=2: their numerators there are respectively 3θ(θ−1)3\theta(\theta-1) and 2θ(2θ−1)(2θ−2)2\theta(2\theta-1)(2\theta-2), both nonzero. Together with a pole of nn, these give at least three distinct points at infinity, contrary to Siegel's theorem.

Let II be the union of the poles of nn and jj alone. It is nonempty and contains at most two geometric points. There are three cases.

Two rational points in II. Choose a rational parameter TT putting them at zero and infinity. Then n,j∈Q[T,T−1]n,j\in\mathbb Q[T,T^{-1}], and at each end at least one of these Laurent polynomials has a pole. For every prime pp, integrality of n,jn,j bounds vp(T)v_p(T) both above and below: as vp(T)v_p(T) tends to either infinity, the term describing the corresponding pole uniquely dominates and has negative valuation. Outside a fixed finite set of primes all nonzero coefficients are units, so these bounds force vp(T)=0v_p(T)=0. At the remaining primes the bounds are fixed finite intervals. Only finitely many rational TT are possible, contrary to the assumed infinite set.

Two conjugate points in II. Along an infinite subsequence nn tends to infinity, so the real points approach a pole of nn. (If both poles are nonreal, nn is bounded on the compact real locus instead.) The bound 0<j/n<1/20<j/n<1/2 makes j/nj/n regular at this pole. Galois conjugation makes it regular at the other pole too. The five-function graph permits no poles elsewhere, because its two possible points at infinity are already in II. Thus j/nj/n is globally regular on P1\mathbb P^1, hence constant, contradicting the preceding paragraph.

One point in II. This point is rational. Put it at infinity, so n=N(T)n=N(T) and j=J(T)j=J(T) are rational polynomials. Passing to a subsequence and changing the sign of TT if needed, we have T→+∞T\to+\infty. The physical inequalities imply deg⁡J≤deg⁡N\deg J\le\deg N, and the ratio J/NJ/N has already been shown to be nonconstant.

Therefore J/NJ/N has a finite pole. There can be only one such geometric point, since infinity is already a pole of nn. Its singleton support is Galois invariant, so it is rational. Translate it to zero. The reduced denominator of J/NJ/N is then a power of TT, giving

N=TrD,J=LD,r≥1,L(0)≠0,deg⁡L≤r.N=T^rD,\qquad J=LD,\qquad r\ge1,\quad L(0)\ne0,\quad\deg L\le r.

The common factor DD is allowed to vanish at zero. In any case N(0)=0N(0)=0. The only possible finite pole of either AA or BB is zero, but their displayed denominators are nonzero there. Hence A,BA,B have no finite poles and are polynomials. The lemma in Section 2 gives the final contradiction. This proves the theorem. □\square

4. The consequence and the remaining gap

The set of bad cubic pairs has the following dichotomy:

  • it is finite; or
  • every infinite subset is Zariski dense in the (n,j)(n,j)-plane.

Thus it now suffices to put all bad pairs in one proper algebraic subset of the plane. The theorem disposes of every curve component of such a subset, including rational curves, with no need to fix or bound uu.

No such global nondensity theorem has been proved here. Therefore this does not yet constrain all bad pairs to a finite exceptional set, even though it proves finiteness on every fixed curve. Nor does it make those curve-wise exceptional sets effective: the proof uses Siegel's theorem and supplies no general height bound. No finite search was used.