Wiki
Wiki

Research notes on every problem, and a library of the papers behind them. Built from the open erdos repository.

Updated

Primitive cubic multiplicity and low-degree geometry


Status

The statements below are proved. They isolate, but do not estimate, the primitive large fibers in the cubic multiplicity problem. No bounded logarithmic moment or positive-density conclusion was obtained.

Removing common dilations costs bounded entropy

Fix positive integral coefficients and F(x)=∑i=13aixi3F(\mathbf x)=\sum_{i=1}^3a_ix_i^3. Let r(n)r(n) count all positive representations and r∗(n)r_*(n) those with gcd⁡(x1,x2,x3)=1\gcd(x_1,x_2,x_3)=1. Define, with 0log⁡0=00\log0=0,

A(X)=∑n≤Xr(n)log⁡r(n),A∗(X)=∑n≤Xr∗(n)log⁡r∗(n).A(X)=\sum_{n\le X}r(n)\log r(n),\qquad A_*(X)=\sum_{n\le X}r_*(n)\log r_*(n).

Then uniformly for sufficiently large XX,

0≤A(X)−∑g≥1A∗(X/g3)≪FX.(1)0\le A(X)-\sum_{g\ge1}A_*(X/g^3)\ll_F X. \tag{1}

To prove this, choose an input uniformly from the finite region {x∈N3:F(x)≤X}\{\mathbf x\in\mathbb N^3:F(\mathbf x)\le X\}, of size T(X)≍FXT(X)\asymp_F X. Put G=gcd⁡(x)G=\gcd(\mathbf x) and Y=F(x)Y=F(\mathbf x). The representations of a fixed nn split into gcd classes of sizes r∗(n/g3)r_*(n/g^3), where g3∣ng^3\mid n. The definition of conditional Shannon entropy therefore gives exactly

A(X)−∑gA∗(X/g3)=T(X)H(G∣Y).A(X)-\sum_g A_*(X/g^3)=T(X)H(G\mid Y).

Also Pr⁡(G=g)≪Fg−3\Pr(G=g)\ll_F g^{-3}, by the box bound for inputs of gcd gg. Consequently Elog⁡G\mathbb E\log G is bounded. Comparing this probability law with qg=g−2/ζ(2)q_g=g^{-2}/\zeta(2) gives H(G)≤log⁡ζ(2)+2Elog⁡G≪F1H(G)\le\log\zeta(2)+2\mathbb E\log G\ll_F1; this is the elementary nonnegativity of relative entropy. Since 0≤H(G∣Y)≤H(G)0\le H(G\mid Y)\le H(G), (1) follows.

In particular, the uniform bounds A(X)≪FXA(X)\ll_F X and A∗(X)≪FXA_*(X)\ll_F X are equivalent. One implication uses r∗(n)≤r(n)r_*(n)\le r(n); the other uses (1) and ∑gg−3<∞\sum_g g^{-3}<\infty. Bounds at small XX can be absorbed into the constant. This is not a statement about transferring a bound given only along one unspecified sparse sequence of scales.

For every fixed 1<p<31<p<3, there is also the equivalence

∑n≤Xr(n)p≪F,pX⟺∑n≤Xr∗(n)p≪F,pX.(2)\sum_{n\le X}r(n)^p\ll_{F,p} X \quad\Longleftrightarrow\quad \sum_{n\le X}r_*(n)^p\ll_{F,p} X. \tag{2}

Indeed r(n)=∑g3∣nr∗(n/g3)r(n)=\sum_{g^3\mid n}r_*(n/g^3), so Minkowski's inequality bounds the ℓp\ell^p norm of rr by a constant times X1/p∑gg−3/pX^{1/p}\sum_g g^{-3/p}. The converse is immediate. Thus common dilations do not account for the missing logarithmic or fractional-moment estimate.

Low-height projected collision planes have negligible input mass

Let EH(N)E_H(N) be the triples in [1,N]3[1,N]^3 lying on a rational plane through the origin whose primitive integral normal has maximum norm at most HH. Then

∣EH(N)∣≪N2H2+NH3.(3)|E_H(N)|\ll N^2H^2+NH^3. \tag{3}

For a primitive normal b\mathbf b of height BB, relabel coordinates so ∣b1∣=B|b_1|=B. Set g=gcd⁡(b2,B)g=\gcd(b_2,B). The congruence b2x2+b3x3≡0(modB)b_2x_2+b_3x_3\equiv0\pmod B forces g∣x3g\mid x_3, since gcd⁡(g,b3)=1\gcd(g,b_3)=1. For each such x3x_3, there is one residue class for x2x_2 modulo B/gB/g. Thus there are at most N2/B+N/g≤N2/B+NN^2/B+N/g\le N^2/B+N possible pairs (x2,x3)(x_2,x_3), and the equation then determines x1x_1. There are O(B2)O(B^2) normals of height BB; summing proves (3).

The fixed-box representation count satisfies RN(n)≤N2R_N(n)\le N^2. For any fixed 0<η<1/20<\eta<1/2, (3) consequently gives

∑x∈EN1/2−η(N)log⁡RN(F(x))≪N3−2ηlog⁡N=o(N3).(4)\sum_{\mathbf x\in E_{N^{1/2-\eta}}(N)} \log R_N(F(\mathbf x)) \ll N^{3-2\eta}\log N=o(N^3). \tag{4}

Every fixed two-parameter homogeneous linear collision identity projects to a fixed rational plane (or a subspace of one) in the input coordinates. Equation (4) removes such identities, and all projected planes in the stated height range, from the logarithmic-moment problem.

This range cannot simply be increased to cover all inputs. Every triple of height at most NN has a nonzero integral orthogonal vector of size O(N)O(\sqrt N): pigeonhole the dot products of vectors in {0,…,L}3\{0,\ldots,L\}^3, with LL a sufficiently large constant times N\sqrt N, into their O(NL)O(NL) possible values, and subtract two equal ones. Dividing by the coordinate gcd makes the normal primitive. High-height planes therefore contain the entire remaining problem, not an automatically negligible exceptional set.

Degrees of curves on the special output surfaces

For n∈Q>0n\in\mathbb Q_{>0} put

Sn:x3+2y3+4z3=nw3⊂PQ3,C=Sn∩{w=0}.S_n:\quad x^3+2y^3+4z^3=nw^3\subset\mathbb P^3_{\mathbb Q}, \qquad C=S_n\cap\{w=0\}.

Proposition. Every curve defined over Q\mathbb Q on SnS_n has degree divisible by 33. In particular, SnS_n contains no rational line or rational conic. No cube-freeness hypothesis on nn is required.

First every closed point of CC has degree divisible by 33. If CC has a point over a finite extension K/Q2K/\mathbb Q_2, let e=vK(2)e=v_K(2) with the valuation normalized integrally. Unless 3∣e3\mid e, the nonzero terms in

x3+2y3+4z3=0x^3+2y^3+4z^3=0

have valuations in distinct classes 0,e,2e(mod3)0,e,2e\pmod3. Their minimum would occur uniquely, which is impossible. Hence 3∣e3\mid e. For a closed point with residue number field LL, apply this at every place vv above 22. Each local degree [Lv:Q2]=evfv[L_v:\mathbb Q_2]=e_vf_v is divisible by 33, and their sum is [L:Q][L:\mathbb Q].

If a curve DD on SnS_n is not contained in w=0w=0, its hyperplane intersection with w=0w=0 is an effective zero-cycle over Q\mathbb Q of degree deg⁡D\deg D, supported on CC. The preceding result makes this degree a multiple of 33. The smooth plane cubic CC itself has degree 33; this also handles curves contained in the boundary and arbitrary curve cycles by additivity.

This excludes degree-one and degree-two curves on individual output surfaces. It does not exclude the split planes on the six-variable collision variety, whose outputs vary along the plane. Nor does it bound the number of higher-degree curves or integral points uniformly as nn varies. Primitive high multiplicity remains uncontrolled.

Three special target cube classes have negligible input mass

For F=x3+2y3+4z3F=x^3+2y^3+4z^3, let E(N)E(N) be the positive triples in [1,N]3[1,N]^3 with F(x)=2em3F(\mathbf x)=2^e m^3 for some e∈{0,1,2}e\in\{0,1,2\} and positive integer mm. Then

∣E(N)∣≪N3(1+log⁡N)4=o(N3).(5)|E(N)|\ll N^{\sqrt3}(1+\log N)^4=o(N^3). \tag{5}

This uses the same checked statement of Salberger's Corollary 0.7 as the coordinate-sharing estimate, not a new uniform surface theorem. For fixed ee, consider the nonsingular diagonal cubic surface

x3+2y3+4z3−2em3=0.x^3+2y^3+4z^3-2^e m^3=0.

A positive solution has no vanishing two-term subsum: a subsum involving only positive terms cannot vanish, and cancellation with the negative term would leave two strictly positive terms summing to zero. Also m≤71/3Nm\le7^{1/3}N, so the projective height is O(N)O(N). The quoted bound gives O(N3(1+log⁡N)4)O(N^{\sqrt3}(1+\log N)^4) primitive points. Summing common dilations gives the same order, since ∑g≥1g−3<∞\sum_{g\ge1}g^{-\sqrt3}<\infty; the additive constant in each primitive bound contributes only O(N)O(N). Summing over the three values of ee proves (5).

As RN(n)≤N2R_N(n)\le N^2, deleting these inputs costs at most 2∣E(N)∣log⁡N=o(N3)2|E(N)|\log N=o(N^3) in the logarithmic-multiplicity sum. This removes only three fixed rational cube classes of targets. It supplies no bound for the remaining integer fibers and no positive-density conclusion.