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Equal radicals of consecutive products

Ruiyi Zhang Independent Researcher, Columbia, Maryland, USA
Abstract.

For every fixed k≥2k\geq 2 and ε>0\varepsilon>0, Fk,k⁢(X)≪k,εX2/3+εF_{k,k}(X)\ll_{k,\varepsilon}X^{2/3+\varepsilon}. For k≥3k\geq 3 this improves the X1+o⁢(1)X^{1+o(1)} bound of Lebowitz–Lockard. For k=2k=2, Kane’s localized estimates give the large-quotient endpoint bound. Our independent proof combines a Pell bound for partner multiplicities, a quotient-tail estimate, and Farey spacing for small quotients. Reuss’s determinant estimate also gives N⁢(H,Y)≪εHε⁢(Y/H+H7/12)N(H,Y)\ll_{\varepsilon}\allowbreak H^{\varepsilon}(Y/H+H^{7/12}), uniformly for H≥2H\geq 2 and 1≤Y<H21\leq Y<H^{2}, where N⁢(H,Y)N(H,Y) counts integers t∈(H,2⁢H]t\in(H,2H] with rad⁡(t⁢(t+1))≤Y\operatorname{rad}(t(t+1))\leq Y. A cubic family gives F⁢(X)≥(41/3/3)⁢X1/3−O⁢(1)F(X)\geq(4^{1/3}/3)X^{1/3}-O(1).

Key words and phrases:
radicals, consecutive integers, Diophantine equations
2020 Mathematics Subject Classification:
Primary 11A25; Secondary 11D25

1. Introduction

For a positive integer aa, let rad⁡(a)=∏p∣ap\operatorname{rad}(a)=\prod_{p\mid a}p. We study the ordered count

F⁢(X)=#⁢{1≤m<n≤X:rad⁡(m⁢(m+1))=rad⁡(n⁢(n+1))}.F(X)=\#\{1\leq m<n\leq X:\operatorname{rad}(m(m+1))=\operatorname{rad}(n(n+1))\}.

More generally, put

Pk⁢(t)=∏j=0k−1(t+j),Fk,k⁢(X)=#⁢{1≤m<n≤X:rad⁡(Pk⁢(m))=rad⁡(Pk⁢(n))}.P_{k}(t)=\prod_{j=0}^{k-1}(t+j),\qquad F_{k,k}(X)=\#\{1\leq m<n\leq X:% \operatorname{rad}(P_{k}(m))=\operatorname{rad}(P_{k}(n))\}.

Thus F⁢(X)=F2,2⁢(X)F(X)=F_{2,2}(X). We impose no disjointness condition on the two blocks, and all implied constants may depend on the fixed integer kk.

Theorem 1.

For every fixed integer k≥2k\geq 2, every ε>0\varepsilon>0, and every real X≥2X\geq 2,

Fk,k⁢(X)≪k,εX2/3+ε.F_{k,k}(X)\ll_{k,\varepsilon}X^{2/3+\varepsilon}.

Erdős asked for the size of F⁢(X)F(X) [3]. Balasubramanian, Shorey and Waldschmidt [1, §5] studied non-overlapping blocks of consecutive integers with the same prime divisors. Lebowitz–Lockard [7, Theorems 5 and 10] proved Fk,k⁢(X)≤X1+o⁢(1)F_{k,k}(X)\leq X^{1+o(1)}. For k≥3k\geq 3, Theorem 1 replaces this exponent by 2/3+ε2/3+\varepsilon. Pell equations of this kind go back to Lehmer’s work on Størmer’s problem [8]; see [1, §2].

For k=2k=2, Kane’s localized estimates [6, Propositions 7 and 10] (Propositions 6 and 9 of [5]) give the large-quotient endpoint bound after specialization to (1,t,−(t+1))(1,t,-(t+1)) and dyadic summation. In the proof below, Lemma 2.4 handles the small-quotient range; together with the endpoint-fibre and quotient-tail bounds, it gives an independent proof of the k=2k=2 case.

Put qk⁢(n)=Pk⁢(n)/rad⁡(Pk⁢(n))q_{k}(n)=P_{k}(n)/\operatorname{rad}(P_{k}(n)). Splitting at a cutoff KK and applying the endpoint-fibre, quotient-tail and small-quotient estimates gives, for max⁡{k,2}≤K≤X\max\{k,2\}\leq K\leq X,

(1.1) Fk,k⁢(X)≪k,εXε⁢(K2+X/K+X1/2).F_{k,k}(X)\ll_{k,\varepsilon}X^{\varepsilon}\bigl{(}K^{2}+X/K+X^{1/2}\bigr{)}.

For X≥k3X\geq k^{3}, taking K=X1/3K=X^{1/3} in (1.1) proves Theorem 1. The bounded range 2≤X<k32\leq X<k^{3} is absorbed into the implied constant, since kk is fixed. Theorem 2 gives an explicit lower-bound family for Erdős’s count. Theorem 3 follows from known estimates; its deduction appears in Appendix A. Section 6 gives two consequences of the pair bound. The tools used for numerical checks and literature searches are identified at the end of the paper.

2. Proof of the fixed-block theorem

Fix an integer k≥2k\geq 2. Put

Pk⁢(n)=∏j=0k−1(n+j),qk⁢(n)=Pk⁢(n)rad⁡(Pk⁢(n)).P_{k}(n)=\prod_{j=0}^{k-1}(n+j),\qquad q_{k}(n)=\frac{P_{k}(n)}{\operatorname{% rad}(P_{k}(n))}.

The function PkP_{k} is positive and strictly increasing on the positive integers. Write ω⁢(D)\omega(D) for the number of distinct prime divisors of DD. All implied constants in this section may depend on kk.

Lemma 2.1 is a Pell-equation count; compare Lebowitz–Lockard [7, Lemma 8] and Tao [11, Lemma 2.10].

Lemma 2.1.

For every squarefree positive integer QQ and every real X≥2X\geq 2,

#⁢{1≤z≤X:rad⁡(z⁢(z+1))∣Q}≪2ω⁢(Q)⁢log⁡(2⁢X),\#\{1\leq z\leq X:\operatorname{rad}(z(z+1))\mid Q\}\ll 2^{\omega(Q)}\log(2X),

with an absolute implied constant. Consequently, for every δ>0\delta>0, every value of rad⁡(Pk⁢(n))\operatorname{rad}(P_{k}(n)) has at most

(2.1) Ck,δ⁢Xk⁢δ⁢log⁡(2⁢X)C_{k,\delta}X^{k\delta}\log(2X)

preimages among the positive integers n≤Xn\leq X.

Proof.

Write z⁢(z+1)=d⁢y2z(z+1)=dy^{2}, where dd is squarefree. Then d∣Qd\mid Q and

(2⁢z+1)2−d⁢(2⁢y)2=1.(2z+1)^{2}-d(2y)^{2}=1.

The case d=1d=1 has no solution with z≥1z\geq 1, since (2⁢z+1−2⁢y)⁢(2⁢z+1+2⁢y)=1(2z+1-2y)(2z+1+2y)=1 is impossible. For a fixed d≥2d\geq 2, put A=2⁢z+1A=2z+1, B=2⁢yB=2y and α=A+B⁢d\alpha=A+B\sqrt{d}. Thus

1<α<2⁢A≤4⁢X+2,α−1=A−B⁢d.1<\alpha<2A\leq 4X+2,\qquad\alpha^{-1}=A-B\sqrt{d}.

If α2>α1\alpha_{2}>\alpha_{1} arise from two solutions, then

α2α1=U0+V0⁢d>1,U0,V0∈ℤ,U02−d⁢V02=1.\frac{\alpha_{2}}{\alpha_{1}}=U_{0}+V_{0}\sqrt{d}>1,\qquad U_{0},V_{0}\in% \mathbb{Z},\qquad U_{0}^{2}-dV_{0}^{2}=1.

Its conjugate is its positive reciprocal. Hence

U0=12⁢(α2α1+α1α2)≥2,α2α1≥2+3.U_{0}=\frac{1}{2}\left(\frac{\alpha_{2}}{\alpha_{1}}+\frac{\alpha_{1}}{\alpha_% {2}}\right)\geq 2,\qquad\frac{\alpha_{2}}{\alpha_{1}}\geq 2+\sqrt{3}.

There are O⁢(log⁡(2⁢X))O(\log(2X)) such solutions for each d∣Qd\mid Q. Summing over the squarefree divisors of QQ proves the first assertion.

For every δ>0\delta>0,

2ω⁢(Q)≪δQδ.2^{\omega(Q)}\ll_{\delta}Q^{\delta}.

Indeed, 2≤pδ2\leq p^{\delta} for all sufficiently large primes pp, and the remaining primes contribute a constant. If Q=rad⁡(Pk⁢(n))Q=\operatorname{rad}(P_{k}(n)) with n≤Xn\leq X, then Q≤(X+k−1)k≪kXkQ\leq(X+k-1)^{k}\ll_{k}X^{k}. Every preimage mm of QQ satisfies rad⁡(m⁢(m+1))∣Q\operatorname{rad}(m(m+1))\mid Q, since k≥2k\geq 2. This gives (2.1). ∎

Erdős and Straus [4, p. 63] also use a Pell equation for products of consecutive integers.

For a positive integer DD, let

ρk⁢(D)=#⁢{xmodD:Pk⁢(x)≡0(modD)}.\rho_{k}(D)=\#\{x\bmod D:P_{k}(x)\equiv 0\pmod{D}\}.
Lemma 2.2.

For every positive integer DD,

ρk⁢(D)≤(k−1)!⁢kω⁢(D).\rho_{k}(D)\leq(k-1)!\,k^{\omega(D)}.
Proof.

If p>k−1p>k-1, the kk factors of PkP_{k} have distinct roots modulo pp. At most one factor is divisible by pp, so ρk⁢(pj)=k\rho_{k}(p^{j})=k for every j≥1j\geq 1.

For p≤k−1p\leq k-1, put Cp=vp⁢((k−1)!)C_{p}=v_{p}((k-1)!). Given an integer xx, choose i∈{0,…,k−1}i\in\{0,\ldots,k-1\} for which vp⁢(x+i)v_{p}(x+i) is maximal, taking vp⁢(0)=∞v_{p}(0)=\infty. For j≠ij\neq i, the ultrametric inequality and maximality give

vp⁢(x+j)≤vp⁢(j−i).v_{p}(x+j)\leq v_{p}(j-i).

Thus

∑j≠ivp⁢(x+j)≤vp⁢(i!⁢(k−1−i)!)≤Cp.\sum_{j\neq i}v_{p}(x+j)\leq v_{p}\bigl{(}i!(k-1-i)!\bigr{)}\leq C_{p}.

If pj∣Pk⁢(x)p^{j}\mid P_{k}(x), then pmax⁡(j−Cp,0)∣x+ip^{\max(j-C_{p},0)}\mid x+i. For each ii there are at most pCpp^{C_{p}} such residue classes modulo pjp^{j}. Hence ρk⁢(pj)≤k⁢pCp\rho_{k}(p^{j})\leq kp^{C_{p}}. The Chinese remainder theorem now gives

ρk⁢(D)≤kω⁢(D)⁢∏p≤k−1pCp=(k−1)!⁢kω⁢(D).∎\rho_{k}(D)\leq k^{\omega(D)}\prod_{p\leq k-1}p^{C_{p}}=(k-1)!\,k^{\omega(D)}.\qed

Sanna [10, Lemma 3.3] proves the related bound Or⁢(x/y1/2)O_{r}(x/y^{1/2}) for the number of n≤xn\leq x such that one of n,…,n+r−1n,\ldots,n+r-1 has powerful part exceeding yy.

Lemma 2.3.

For all real X≥2X\geq 2, K≥max⁡(k,2)K\geq\max(k,2) and 0<η<10<\eta<1,

(2.2) #⁢{1≤n≤X:qk⁢(n)>K}≪k,ηX⁢K−1+η+K2⁢(1+log⁡K)k−1+X1/2.\#\{1\leq n\leq X:q_{k}(n)>K\}\ll_{k,\eta}XK^{-1+\eta}+K^{2}(1+\log K)^{k-1}+X% ^{1/2}.
Proof.

Let 1≤n≤X1\leq n\leq X satisfy qk⁢(n)>Kq_{k}(n)>K. Suppose first that a prime p>Kp>K divides qk⁢(n)q_{k}(n). Then p2∣Pk⁢(n)p^{2}\mid P_{k}(n). Since p>K≥kp>K\geq k, exactly one factor is divisible by pp, and p2∣n+ip^{2}\mid n+i for some 0≤i<k0\leq i<k. The number of these nn is at most

k⁢∑K<p≤X+k−1(Xp2+1)≪kXK+X1/2.k\sum_{K<p\leq\sqrt{X+k-1}}\left(\frac{X}{p^{2}}+1\right)\ll_{k}\frac{X}{K}+X^% {1/2}.

The last bound follows by summing over all integers in place of primes.

Otherwise every prime factor of qk⁢(n)q_{k}(n) is at most KK. Multiply its prime factors, with multiplicity, until the product first exceeds KK. This gives an integer gg such that

g∣qk⁢(n),K⁢<g≤K2,g⁢rad⁡(g)∣⁢Pk⁢(n).g\mid q_{k}(n),\qquad K<g\leq K^{2},\qquad g\operatorname{rad}(g)\mid P_{k}(n).

For the last divisibility, if pa∣gp^{a}\mid g, then a≤vp⁢(Pk⁢(n))−1a\leq v_{p}(P_{k}(n))-1. Lemma 2.2 bounds the number of these nn by

(2.3) (k−1)!⁢∑K<g≤K2kω⁢(g)⁢(Xg⁢rad⁡(g)+1).(k-1)!\sum_{K<g\leq K^{2}}k^{\omega(g)}\left(\frac{X}{g\operatorname{rad}(g)}+% 1\right).

For 0<η<10<\eta<1, the Euler product

∑g≥1kω⁢(g)⁢g1−ηg⁢rad⁡(g)=∏p(1+kp⁢(pη−1))\sum_{g\geq 1}\frac{k^{\omega(g)}g^{1-\eta}}{g\operatorname{rad}(g)}=\prod_{p}% \left(1+\frac{k}{p(p^{\eta}-1)}\right)

converges, since its local factor is 1+Ok,η⁢(p−1−η)1+O_{k,\eta}(p^{-1-\eta}). The first term of (2.3) is therefore Ok,η⁢(X⁢K−1+η)O_{k,\eta}(XK^{-1+\eta}).

Let τk⁢(g)\tau_{k}(g) count the ordered factorizations of gg into kk positive integers. Then kω⁢(g)≤τk⁢(g)k^{\omega(g)}\leq\tau_{k}(g) and, for Y≥1Y\geq 1,

∑g≤Yτk⁢(g)≤Y⁢(∑r≤Y1r)k−1≤Y⁢(1+log⁡Y)k−1.\sum_{g\leq Y}\tau_{k}(g)\leq Y\left(\sum_{r\leq Y}\frac{1}{r}\right)^{k-1}% \leq Y(1+\log Y)^{k-1}.

The second term of (2.3) is Ok⁢(K2⁢(1+log⁡K)k−1)O_{k}(K^{2}(1+\log K)^{k-1}). This proves (2.2). ∎

Lemma 2.4.

For every real X≥2X\geq 2 and K≥1K\geq 1,

#⁢{(m,n):1≤m<n≤X,qk⁢(m),qk⁢(n)≤K,rad⁡(Pk⁢(m))=rad⁡(Pk⁢(n))}≪kK2⁢log⁡(2⁢X).\#\left\{(m,n):\begin{gathered}1\leq m<n\leq X,\quad q_{k}(m),q_{k}(n)\leq K,% \\ \operatorname{rad}(P_{k}(m))=\operatorname{rad}(P_{k}(n))\end{gathered}\right% \}\ll_{k}K^{2}\log(2X).
Proof.

Put μ=qk⁢(m)\mu=q_{k}(m) and ν=qk⁢(n)\nu=q_{k}(n). Strict monotonicity of PkP_{k} gives

(2.4) 1≤μ<ν≤K,ν⁢Pk⁢(m)=μ⁢Pk⁢(n).1\leq\mu<\nu\leq K,\qquad\nu P_{k}(m)=\mu P_{k}(n).

Set

ξ=2⁢m+k−1,ζ=2⁢n+k−1,Rk⁢(U)=∏j=0k−1(U+2⁢j−k+1).\xi=2m+k-1,\qquad\zeta=2n+k-1,\qquad R_{k}(U)=\prod_{j=0}^{k-1}(U+2j-k+1).

Then Rk⁢(ζ)=2k⁢Pk⁢(n)R_{k}(\zeta)=2^{k}P_{k}(n). With

ℋk={h:1≤h≤k−1,h≡k−1(mod2)},Ak=∑h∈ℋkh2,\mathcal{H}_{k}=\{h:1\leq h\leq k-1,\ h\equiv k-1\pmod{2}\},\qquad A_{k}=\sum_% {h\in\mathcal{H}_{k}}h^{2},

we have

Rk⁢(U)=Uk⁢Gk⁢(U),Gk⁢(U)=∏h∈ℋk(1−h2U2).R_{k}(U)=U^{k}G_{k}(U),\qquad G_{k}(U)=\prod_{h\in\mathcal{H}_{k}}\left(1-% \frac{h^{2}}{U^{2}}\right).

For U≥k+1U\geq k+1, the function GkG_{k} is strictly increasing and

(2.5) 0<Gk⁢(U)<1,1−Gk⁢(U)≤AkU2.0<G_{k}(U)<1,\qquad 1-G_{k}(U)\leq\frac{A_{k}}{U^{2}}.

Indeed, ℋk\mathcal{H}_{k} is nonempty and each factor is positive and strictly increasing. The last inequality follows from 1−∏j(1−xj)≤∑jxj1-\prod_{j}(1-x_{j})\leq\sum_{j}x_{j} for 0≤xj≤10\leq x_{j}\leq 1.

Fix μ,ν\mu,\nu in (2.4), and put γ=(ν/μ)1/k\gamma=(\nu/\mu)^{1/k} and λ=ζ/ξ\lambda=\zeta/\xi. Thus ζ>ξ≥k+1\zeta>\xi\geq k+1 and

γk=λk⁢Gk⁢(ζ)Gk⁢(ξ),1<λ<γ.\gamma^{k}=\lambda^{k}\frac{G_{k}(\zeta)}{G_{k}(\xi)},\qquad 1<\lambda<\gamma.

Using (2.5), we obtain

0<γ−λ\displaystyle 0<\gamma-\lambda =γ⁢(1−(Gk⁢(ξ)Gk⁢(ζ))1/k)\displaystyle=\gamma\left(1-\left(\frac{G_{k}(\xi)}{G_{k}(\zeta)}\right)^{1/k}\right)
≤γ⁢(1−Gk⁢(ξ)1/k)\displaystyle\leq\gamma\bigl{(}1-G_{k}(\xi)^{1/k}\bigr{)}
≤γ⁢(1−Gk⁢(ξ))\displaystyle\leq\gamma\bigl{(}1-G_{k}(\xi)\bigr{)}
≤Ak⁢γξ2.\displaystyle\leq\frac{A_{k}\gamma}{\xi^{2}}.

Write λ=h/q\lambda=h/q in lowest terms, with h,q>0h,q>0. Since q∣ξq\mid\xi,

0<γ−hq≤Ak⁢γq2,q≤2⁢X+k−1.0<\gamma-\frac{h}{q}\leq\frac{A_{k}\gamma}{q^{2}},\qquad q\leq 2X+k-1.

In a block 2j≤q<2j+12^{j}\leq q<2^{j+1}, these fractions lie in an interval of length Ak⁢γ/22⁢jA_{k}\gamma/2^{2j}. Distinct reduced fractions in the block are more than 2−2⁢j−22^{-2j-2} apart. There are at most 1+4⁢Ak⁢γ1+4A_{k}\gamma fractions in each block, and hence Ok⁢(γ⁢log⁡(2⁢X))O_{k}(\gamma\log(2X)) possible values of λ\lambda.

For each such λ\lambda, every possible ξ\xi is a root of

ν⁢Rk⁢(U)−μ⁢Rk⁢(λ⁢U)=0.\nu R_{k}(U)-\mu R_{k}(\lambda U)=0.

This polynomial has degree kk, since its leading coefficient is ν−μ⁢λk=μ⁢(γk−λk)>0\nu-\mu\lambda^{k}=\mu(\gamma^{k}-\lambda^{k})>0. It has at most kk real roots. Each root determines at most one pair (m,n)(m,n). Therefore, for fixed μ,ν\mu,\nu, the number of pairs in (2.4) is

≪k(ν/μ)1/k⁢log⁡(2⁢X).\ll_{k}(\nu/\mu)^{1/k}\log(2X).

Finally,

∑1≤μ<ν≤K(ν/μ)1/k≤∑ν≤Kν1/k⁢kk−1⁢ν1−1/k≪kK2.∎\sum_{1\leq\mu<\nu\leq K}(\nu/\mu)^{1/k}\leq\sum_{\nu\leq K}\nu^{1/k}\frac{k}{% k-1}\nu^{1-1/k}\ll_{k}K^{2}.\qed
Proof of Theorem 1.

Let ε>0\varepsilon>0. A counted pair either has both quotients at most KK, or has an endpoint in the exceptional set of Lemma 2.3. Multiplying the latter count by (2.1) and applying Lemma 2.4 gives, for K≥max⁡(k,2)K\geq\max(k,2),

Fk,k⁢(X)≪k,δ,η\displaystyle F_{k,k}(X)\ll_{k,\delta,\eta}{} K2⁢log⁡(2⁢X)\displaystyle K^{2}\log(2X)
(2.6) +Xk⁢δ⁢log⁡(2⁢X)⁢(X⁢K−1+η+K2⁢(1+log⁡K)k−1+X1/2).\displaystyle+X^{k\delta}\log(2X)\left(XK^{-1+\eta}+K^{2}(1+\log K)^{k-1}+X^{1% /2}\right).

The fibre bound counts all possible partners 1≤m≤X1\leq m\leq X, so this also covers pairs whose smaller endpoint is exceptional.

Ignoring the factors Xk⁢δX^{k\delta}, KηK^{\eta} and the logarithms, K=XτK=X^{\tau} gives the exponent max⁡(2⁢τ,1−τ,1/2)\max(2\tau,1-\tau,1/2), minimized at τ=1/3\tau=1/3. Set K=max⁡(k,2,X1/3)K=\max(k,2,X^{1/3}). If X≥k3X\geq k^{3}, then K=X1/3K=X^{1/3}. With this choice fixed, take

η=min⁡(12,ε2),δ=ε4⁢k.\eta=\min\left(\frac{1}{2},\frac{\varepsilon}{2}\right),\qquad\delta=\frac{% \varepsilon}{4k}.

Every power of XX in (2) is at most

23+k⁢δ+η3≤23+5⁢ε12.\frac{2}{3}+k\delta+\frac{\eta}{3}\leq\frac{2}{3}+\frac{5\varepsilon}{12}.

The logarithmic factors together are Ok,ε⁢(Xε/2)O_{k,\varepsilon}(X^{\varepsilon/2}). Hence

Fk,k⁢(X)≪k,εX2/3+ε.F_{k,k}(X)\ll_{k,\varepsilon}X^{2/3+\varepsilon}.

The bounded range 2≤X<k32\leq X<k^{3} is absorbed into the implied constant. ∎

3. A cubic lower-bound family

Theorem 2.

There is an absolute constant CC such that, for every real X≥2X\geq 2,

F⁢(X)≥41/33⁢X1/3−C.F(X)\geq\frac{4^{1/3}}{3}X^{1/3}-C.
Proof.

Erdős posed the product-support counting problem in [3]. We know of no published source for this particular polynomial family. Take integers t≥7t\geq 7 satisfying

t≢0(mod4),t≡1,2,7,8(mod9),t\not\equiv 0\pmod{4},\qquad t\equiv 1,2,7,8\pmod{9},

and put

m=t2−43,n=t3−3⁢t−24.m=\frac{t^{2}-4}{3},\qquad n=\frac{t^{3}-3t-2}{4}.

The resulting integers are positive, and

12⁢(n−m)=3⁢t3−4⁢t2−9⁢t+10>012(n-m)=3t^{3}-4t^{2}-9t+10>0

for t≥7t\geq 7, so m<nm<n. Direct multiplication gives

m⁢(m+1)=(t2−4)⁢(t2−1)9,n⁢(n+1)=(t2−4)⁢(t2−1)216.m(m+1)=\frac{(t^{2}-4)(t^{2}-1)}{9},\qquad n(n+1)=\frac{(t^{2}-4)(t^{2}-1)^{2}% }{16}.

For every prime other than 22 and 33, the two products have the same prime support. If t≡±1(mod9)t\equiv\pm 1\pmod{9}, then 9∣t2−19\mid t^{2}-1 and 3∣t2−43\mid t^{2}-4; if t≡±2(mod9)t\equiv\pm 2\pmod{9}, then 9∣t2−49\mid t^{2}-4 and 3∣t2−13\mid t^{2}-1. Thus division by 99 leaves a factor 33 in the first product, and the second product is also divisible by 33.

If tt is odd, then 8∣t2−18\mid t^{2}-1, so both products remain even after their displayed divisions. If t≡2(mod4)t\equiv 2\pmod{4}, then 32∣t2−432\mid t^{2}-4, which again leaves both products even after division by 1616. Hence the two products have equal radicals.

The conditions specify twelve residue classes modulo 3636, of density 1/31/3. Since n=t3/4+O⁢(t)n=t^{3}/4+O(t), the number of such tt with n≤Xn\leq X is (41/3/3)⁢X1/3+O⁢(1)(4^{1/3}/3)X^{1/3}+O(1). The map t↦mt\mapsto m is strictly increasing for t≥7t\geq 7, so these give distinct pairs counted by F⁢(X)F(X). ∎

4. A radical-threshold estimate from known results

For real H≥2H\geq 2 and 1≤Y<H21\leq Y<H^{2}, define

N⁢(H,Y)=#⁢{t∈ℤ:H<t≤2⁢H,rad⁡(t⁢(t+1))≤Y}.N(H,Y)=\#\{t\in\mathbb{Z}:H<t\leq 2H,\operatorname{rad}(t(t+1))\leq Y\}.
Theorem 3.

For every ε>0\varepsilon>0,

N⁢(H,Y)≪εHε⁢(YH+H7/12)N(H,Y)\ll_{\varepsilon}H^{\varepsilon}\left(\frac{Y}{H}+H^{7/12}\right)

uniformly for real H≥2H\geq 2 and 1≤Y<H21\leq Y<H^{2}.

Theorem 3 is a consequence of known estimates, stated here in this notation. In the proof of Kane’s Proposition 7 [6], the dyadic lattice count for triples of height N0N_{0} is bounded by

N0ε⁢[rad⁡(A)⁢rad⁡(B)⁢rad⁡(C)|C|+v⁢(A)⁢v⁢(B)⁢v⁢(C)].N_{0}^{\varepsilon}\left[\frac{\operatorname{rad}(A)\operatorname{rad}(B)% \operatorname{rad}(C)}{|C|}+v(A)v(B)v(C)\right].

For H<t≤2⁢HH<t\leq 2H, take N0=⌈2⁢H+1⌉N_{0}=\lceil 2H+1\rceil and (A,B,C)=(1,t,−(t+1))(A,B,C)=(1,t,-(t+1)). Put

S2⁢(n)=∏pj∥np⌊j/2⌋,T2⁢(n)=nS2⁢(n)2,Π=S2⁢(t)⁢S2⁢(t+1).S_{2}(n)=\prod_{p^{j}\parallel n}p^{\lfloor j/2\rfloor},\qquad T_{2}(n)=\frac{% n}{S_{2}(n)^{2}},\qquad\Pi=S_{2}(t)S_{2}(t+1).

Here v⁢(n)=∏p2∣np=rad⁡(S2⁢(n))v(n)=\prod_{p^{2}\mid n}p=\operatorname{rad}(S_{2}(n)) in Kane’s notation. When Π≤H2/3\Pi\leq H^{2/3}, the displayed lattice inequality gives Hε⁢(Y/H+Π)H^{\varepsilon}(Y/H+\Pi). For Π>H2/3\Pi>H^{2/3}, Kane’s Proposition 10 [6, Proposition 10] gives the square-part estimate

Hε⁢(T2⁢(t)⁢T2⁢(t+1)+Π⁢T2⁢(t)⁢T2⁢(t+1))≪Hε⁢(H2Π2+HΠ),H^{\varepsilon}\left(T_{2}(t)T_{2}(t+1)+\sqrt{\Pi T_{2}(t)T_{2}(t+1)}\right)% \ll H^{\varepsilon}\left(\frac{H^{2}}{\Pi^{2}}+\frac{H}{\sqrt{\Pi}}\right),

since t⁢(t+1)≪H2t(t+1)\ll H^{2}. Both ranges are Oε⁢(Hε⁢(Y/H+H2/3))O_{\varepsilon}(H^{\varepsilon}(Y/H+H^{2/3})), with the split point Π=H2/3\Pi=H^{2/3} balancing the terms in Kane’s proof. Diao’s Lemma 2.1 [2] gives the 7/127/12 estimate in the large-product range. Appendix A gives a detailed deduction via Reuss’s theorem. Theorem 3 records this known consequence in the notation used here.

5. Lebowitz–Lockard’s Conjecture 11

Lebowitz–Lockard state the following conjecture [7, Conjecture 11]:

If k,ℓ>1k,\ell>1 and (k,ℓ)≠(2,2)(k,\ell)\neq(2,2), then the equation

rad⁡(m⁢(m+1)⁢⋯⁢(m+k−1))=rad⁡(n⁢(n+1)⁢⋯⁢(n+ℓ−1))\operatorname{rad}(m(m+1)\cdots(m+k-1))=\operatorname{rad}(n(n+1)\cdots(n+\ell% -1))

only has finitely many solutions.

Their preceding definition of Fk,ℓF_{k,\ell} imposes m<nm<n. The conjecture also fails under this order condition, for (k,ℓ)=(3,2)(k,\ell)=(3,2) and (4,2)(4,2). Equivalent forms of the identities below appear in Erdős–Straus [4, p. 64]. For every positive integer tt,

P2⁢(t⁢(t+2))\displaystyle P_{2}(t(t+2)) =t⁢(t+2)⁢(t+1)2,\displaystyle=t(t+2)(t+1)^{2},
P2⁢(t⁢(t+3)2)\displaystyle P_{2}\!\left(\frac{t(t+3)}{2}\right) =14⁢P4⁢(t).\displaystyle=\frac{1}{4}P_{4}(t).

Since t+1∣P3⁢(t)t+1\mid P_{3}(t), the first identity shows that (m,n)=(t,t⁢(t+2))(m,n)=(t,t(t+2)) gives equal radicals for (k,ℓ)=(3,2)(k,\ell)=(3,2). For the second identity, four consecutive integers have product divisible by 2424: one is divisible by 44, a distinct one is even, and one is divisible by 33. Thus P4⁢(t)/4P_{4}(t)/4 remains divisible by 66, so division by 44 leaves its prime support unchanged. The integer t⁢(t+3)/2t(t+3)/2 is integral, and the second identity gives equal radicals for (m,n)=(t,t⁢(t+3)/2)(m,n)=(t,t(t+3)/2) and (k,ℓ)=(4,2)(k,\ell)=(4,2). Both families have m<nm<n for every positive integer tt. Swapping the variables gives infinite families for (2,3)(2,3) and (2,4)(2,4) if no order condition is imposed. Conjecture 11 is false as literally stated; its intended form is unclear. Erdős and Straus [4, p. 64] conjectured that A⁢(n,k)=ρ⁢A⁢(m,ℓ)A(n,k)=\rho A(m,\ell) has only finitely many solutions with m≥n+km\geq n+k for each rational ρ\rho when min⁡(k,ℓ)>1\min(k,\ell)>1 and max⁡(k,ℓ)>2\max(k,\ell)>2, where A⁢(n,k)=(n+k)!/n!A(n,k)=(n+k)!/n!. The second identity reads A⁢(t−1,4)=4⁢A⁢(t⁢(t+3)/2−1,2)A(t-1,4)=4A(t(t+3)/2-1,2), and t⁢(t+3)/2−1>(t−1)+4t(t+3)/2-1>(t-1)+4 for every integer t≥3t\geq 3. Their conjecture is therefore also false as literally stated. They print the underlying four-factor identity on the same page in their divisibility argument.

6. Further consequences

6.1. Radical fibres and moments

Remark 6.1.

Lemma 2.1 is a growth form of the Pell argument; compare Lehmer [8, Theorem 1] and Lebowitz–Lockard [7, Lemma 8]. In particular, if

νR⁢(X)=#⁢{1≤n≤X:rad⁡(n⁢(n+1))=R},\nu_{R}(X)=\#\{1\leq n\leq X:\operatorname{rad}(n(n+1))=R\},

then Lemma 2.1 gives

νR⁢(X)≪2ω⁢(R)⁢log⁡(2⁢X)≪εXε(R≪X2),\nu_{R}(X)\ll 2^{\omega(R)}\log(2X)\ll_{\varepsilon}X^{\varepsilon}\qquad(R\ll X% ^{2}),

so maxR⁡νR⁢(X)≪εXε\max_{R}\nu_{R}(X)\ll_{\varepsilon}X^{\varepsilon}. Since

∑RνR⁢(X)=⌊X⌋,∑RνR⁢(X)⁢(νR⁢(X)−1)=2⁢F⁢(X),\sum_{R}\nu_{R}(X)=\lfloor X\rfloor,\qquad\sum_{R}\nu_{R}(X)(\nu_{R}(X)-1)=2F(% X),

the main theorem gives

#⁢{rad⁡(n⁢(n+1)):1≤n≤X}\displaystyle\#\{\operatorname{rad}(n(n+1)):1\leq n\leq X\} =⌊X⌋−Oε⁢(X2/3+ε),\displaystyle=\lfloor X\rfloor-O_{\varepsilon}(X^{2/3+\varepsilon}),
∑RνR⁢(X)r\displaystyle\sum_{R}\nu_{R}(X)^{r} =⌊X⌋+Or,ε⁢(X2/3+ε)\displaystyle=\lfloor X\rfloor+O_{r,\varepsilon}(X^{2/3+\varepsilon})

for each fixed integer r≥2r\geq 2. For r≥3r\geq 3, summing the following pointwise bound over RR gives

0≤νR⁢(X)r−νR⁢(X)≤(r−1)⁢(maxS⁡νS⁢(X))r−2⁢νR⁢(X)⁢(νR⁢(X)−1),0\leq\nu_{R}(X)^{r}-\nu_{R}(X)\leq(r-1)\bigl{(}\max_{S}\nu_{S}(X)\bigr{)}^{r-2% }\nu_{R}(X)(\nu_{R}(X)-1),

and hence the stated moment estimate. The case r=2r=2 follows from the pair identity above. That identity also gives

0≤⌊X⌋−#⁢{R:νR⁢(X)>0}=∑νR⁢(X)>0(νR⁢(X)−1)≤F⁢(X).0\leq\lfloor X\rfloor-\#\{R:\nu_{R}(X)>0\}=\sum_{\nu_{R}(X)>0}(\nu_{R}(X)-1)% \leq F(X).

6.2. Short gaps

Remark 6.2.

For 1≤Δ≤X1\leq\Delta\leq X, let G⁢(X,Δ)G(X,\Delta) count the pairs in F⁢(X)F(X) with n−m≤Δn-m\leq\Delta. For a fixed gap d=n−m≥2d=n-m\geq 2, every prime dividing the common radical divides one factor from each of m⁢(m+1)m(m+1) and n⁢(n+1)n(n+1). Subtracting these factors shows that it divides one of d−1,d,d+1d-1,d,d+1. There are at most 2ω⁢(d⁢(d−1)⁢(d+1))2^{\omega(d(d-1)(d+1))} possible common radicals. Since d⁢(d−1)⁢(d+1)≤X3d(d-1)(d+1)\leq X^{3}, take δ=ε/6\delta=\varepsilon/6 in 2ω⁢(q)≪δqδ2^{\omega(q)}\ll_{\delta}q^{\delta}. This contributes at most Oε⁢(Xε/2)O_{\varepsilon}(X^{\varepsilon/2}) radicals. In the fibre estimate, take its exponent parameter to be ε/8\varepsilon/8; then Xε/4⁢log⁡(2⁢X)≪εXε/2X^{\varepsilon/4}\log(2X)\ll_{\varepsilon}X^{\varepsilon/2}. Thus each gap contributes Oε⁢(Xε)O_{\varepsilon}(X^{\varepsilon}) pairs. Summing over d≤Δd\leq\Delta gives

G⁢(X,Δ)≪εΔ⁢Xε.G(X,\Delta)\ll_{\varepsilon}\Delta X^{\varepsilon}.

For d=1d=1, equality of radicals reduces to rad⁡(m)=rad⁡(m+2)\operatorname{rad}(m)=\operatorname{rad}(m+2), which forces m=2m=2 and gives the single pair (m,n)=(2,3)(m,n)=(2,3): their common radical divides rad⁡(gcd⁡(m,m+2))∣2\operatorname{rad}(\gcd(m,m+2))\mid 2. It cannot be 11, so both terms are powers of 22, which leaves m=2m=2.

Appendix A Proof of Theorem 3

Proof of Theorem 3.

Write uniquely

t=d2⁢r,t+1=f2⁢s,t=d^{2}r,\qquad t+1=f^{2}s,

where r,sr,s are squarefree positive integers. Then

(A.1) f2⁢s−d2⁢r=1,(d,f)=(r,s)=1.f^{2}s-d^{2}r=1,\qquad(d,f)=(r,s)=1.

Put

α0=gcd⁡(r,rad⁡(d)),β0=gcd⁡(s,rad⁡(f)).\alpha_{0}=\gcd(r,\operatorname{rad}(d)),\qquad\beta_{0}=\gcd(s,\operatorname{% rad}(f)).

The radical identity is

(A.2) rad⁡(t⁢(t+1))=r⁢s⁢rad⁡(d)⁢rad⁡(f)α0⁢β0.\operatorname{rad}(t(t+1))=\frac{rs\operatorname{rad}(d)\operatorname{rad}(f)}% {\alpha_{0}\beta_{0}}.

Since r⁢s>H2/(d2⁢f2)rs>H^{2}/(d^{2}f^{2}), every point counted by N⁢(H,Y)N(H,Y) satisfies

(A.3) d2⁢f2⁢α0⁢β0≥H2⁢rad⁡(d)⁢rad⁡(f)Y.d^{2}f^{2}\alpha_{0}\beta_{0}\geq\frac{H^{2}\operatorname{rad}(d)\operatorname% {rad}(f)}{Y}.

Set H0=H7/12H_{0}=H^{7/12} and first count the points with d⁢f≤H0df\leq H_{0}. For fixed d,f,α0,β0d,f,\alpha_{0},\beta_{0}, the divisibilities α0∣r\alpha_{0}\mid r and β0∣s\beta_{0}\mid s give

t≡0(modd2⁢α0),t≡−1(modf2⁢β0).t\equiv 0\pmod{d^{2}\alpha_{0}},\qquad t\equiv-1\pmod{f^{2}\beta_{0}}.

The moduli are coprime, since every prime dividing the first divides tt and every prime dividing the second divides t+1t+1. Thus the Chinese remainder theorem gives at most one class modulo d2⁢f2⁢α0⁢β0d^{2}f^{2}\alpha_{0}\beta_{0}, containing at most H/(d2⁢f2⁢α0⁢β0)+1H/(d^{2}f^{2}\alpha_{0}\beta_{0})+1 integers in the interval. By (A.3),

(A.4) Nlo≪YH⁢∑d⁢f≤H0τ⁢(rad⁡(d))⁢τ⁢(rad⁡(f))rad⁡(d)⁢rad⁡(f)+∑d⁢f≤H0τ⁢(d)⁢τ⁢(f).N_{\mathrm{lo}}\ll\frac{Y}{H}\sum_{df\leq H_{0}}\frac{\tau(\operatorname{rad}(% d))\tau(\operatorname{rad}(f))}{\operatorname{rad}(d)\operatorname{rad}(f)}+% \sum_{df\leq H_{0}}\tau(d)\tau(f).

For every η>0\eta>0, Rankin’s trick and the convergent product

∑n≥1τ⁢(rad⁡(n))rad⁡(n)⁢nη=∏p(1+2p⁢(pη−1))<∞\sum_{n\geq 1}\frac{\tau(\operatorname{rad}(n))}{\operatorname{rad}(n)n^{\eta}% }=\prod_{p}\left(1+\frac{2}{p(p^{\eta}-1)}\right)<\infty

give

∑d⁢f≤H0τ⁢(rad⁡(d))⁢τ⁢(rad⁡(f))rad⁡(d)⁢rad⁡(f)≪ηH0η.\sum_{df\leq H_{0}}\frac{\tau(\operatorname{rad}(d))\tau(\operatorname{rad}(f)% )}{\operatorname{rad}(d)\operatorname{rad}(f)}\ll_{\eta}H_{0}^{\eta}.

Also ∑d⁢f≤H0τ⁢(d)⁢τ⁢(f)≪H0⁢(log⁡(2⁢H0))3\sum_{df\leq H_{0}}\tau(d)\tau(f)\ll H_{0}(\log(2H_{0}))^{3}, by summing the four-fold divisor function. Taking η\eta sufficiently small in terms of ε\varepsilon and absorbing logarithms gives

(A.5) Nlo≪εHε⁢(YH+H7/12).N_{\mathrm{lo}}\ll_{\varepsilon}H^{\varepsilon}\left(\frac{Y}{H}+H^{7/12}% \right).

It remains to count solutions of (A.1) with d⁢f>H0df>H_{0}; here we discard the radical restriction. Since r,s≥1r,s\geq 1, t≤2⁢Ht\leq 2H, and t+1≤3⁢Ht+1\leq 3H, we have

(A.6) d≤2⁢H,f≤3⁢H.d\leq\sqrt{2H},\qquad f\leq\sqrt{3H}.

Partition the d,fd,f ranges into dyadic boxes and refine each into multiplicative cells of ratio λ=21/8\lambda=2^{1/8}. On a cell write

S<t≤λ⁢S,𝒟<d≤λ⁢𝒟,ℰ<f≤λ⁢ℰ,S<t\leq\lambda S,\qquad\mathcal{D}<d\leq\lambda\mathcal{D},\qquad\mathcal{E}<f% \leq\lambda\mathcal{E},

and put x=S/λ2x=S/\lambda^{2}, U=x/𝒟2U=x/\mathcal{D}^{2}, and V=x/ℰ2V=x/\mathcal{E}^{2}. Then r=t/d2∈(U,λ3⁢U)r=t/d^{2}\in(U,\lambda^{3}U) and s=(t+1)/f2∈(V,λ3⁢V+ℰ−2)s=(t+1)/f^{2}\in(V,\lambda^{3}V+\mathcal{E}^{-2}). Since λ3+λ2/S<2\lambda^{3}+\lambda^{2}/S<2 for S≥2S\geq 2, we have

U<r<2⁢U,V<s<2⁢V,U<r<2U,\qquad V<s<2V,

and the variables lie in dyadic boxes with the exact scale identities

U⁢𝒟2=V⁢ℰ2=x≍H.U\mathcal{D}^{2}=V\mathcal{E}^{2}=x\asymp H.

Only a bounded number of such cells is used in each dyadic box. In every cell,

(A.7) U⁢V≍H2(𝒟⁢ℰ)2.UV\asymp\frac{H^{2}}{(\mathcal{D}\mathcal{E})^{2}}.

Suppose first that U⁢V≤H1/2UV\leq H^{1/2}. Fix squarefree r,sr,s. If r⁢s=1rs=1, (A.1) would give f2−d2=1f^{2}-d^{2}=1, which is impossible for positive d,fd,f. Otherwise

(s⁢f)2−r⁢s⁢d2=s.(sf)^{2}-rsd^{2}=s.

The element

ξ=s⁢f+d⁢r⁢s=s⁢(t+1+t)\xi=sf+d\sqrt{rs}=\sqrt{s}\bigl{(}\sqrt{t+1}+\sqrt{t}\bigr{)}

is totally positive and has norm ss. The relevant quadratic order is maximal unless r⁢s≡1(mod4)rs\equiv 1\pmod{4}; in that case it has conductor 22, and ss is odd and coprime to the conductor. Thus the ideals of norm ss in the order are invertible and correspond to ideals of norm ss in the maximal order. Every prime dividing ss ramifies, so at most τ⁢(s)\tau(s) such ideals arise. Generators of the same principal ideal differ by a unit of the order; for two totally positive generators their ratio is a totally positive norm-one unit. If ϵ>1\epsilon>1 is such a unit, its integer trace is at least 33, whence ϵ≥(3+5)/2>2\epsilon\geq(3+\sqrt{5})/2>2. In contrast, the displayed formula for ξ\xi shows that its ratio across H<t≤2⁢HH<t\leq 2H is less than 2\sqrt{2}. Thus each ideal contributes at most one solution. Since s≤3⁢Hs\leq 3H, τ⁢(s)≪εHε\tau(s)\ll_{\varepsilon}H^{\varepsilon}. There are O⁢(U⁢V)O(UV) choices of r,sr,s in their boxes, and therefore

(A.8) NU⁢V≤H1/2≪εHε⁢U⁢V≪εH1/2+ε.N_{UV\leq H^{1/2}}\ll_{\varepsilon}H^{\varepsilon}UV\ll_{\varepsilon}H^{1/2+% \varepsilon}.

Now suppose U⁢V>H1/2UV>H^{1/2}. Equations (A.7) and d⁢f>H0df>H_{0} give

H7/12≪𝒟⁢ℰ≪H3/4,log⁡(𝒟⁢ℰ)≍log⁡(U⁢V)≍log⁡H.H^{7/12}\ll\mathcal{D}\mathcal{E}\ll H^{3/4},\qquad\log(\mathcal{D}\mathcal{E}% )\asymp\log(UV)\asymp\log H.

Apply Reuss’s determinant estimate [9, Theorem 1] to s⁢f2−r⁢d2=1sf^{2}-rd^{2}=1 with (k,ℓ,h)=(2,1,1)(k,\ell,h)=(2,1,1) and scales U=x/𝒟2U=x/\mathcal{D}^{2}, V=x/ℰ2V=x/\mathcal{E}^{2}. They satisfy U⁢𝒟2=V⁢ℰ2=xU\mathcal{D}^{2}=V\mathcal{E}^{2}=x. Since d⁢f>H0df>H_{0} and (A.6) gives d≤2⁢Hd\leq\sqrt{2H} and f≤3⁢Hf\leq\sqrt{3H}, we have

d>H0/3⁢H≫H1/12,f>H0/2⁢H≫H1/12.d>H_{0}/\sqrt{3H}\gg H^{1/12},\qquad f>H_{0}/\sqrt{2H}\gg H^{1/12}.

As d≤λ⁢𝒟d\leq\lambda\mathcal{D}, f≤λ⁢ℰf\leq\lambda\mathcal{E}, and x≍Hx\asymp H, this implies 𝒟,ℰ,x>1\mathcal{D},\mathcal{E},x>1 for large HH. Define

M=exp⁡(9⁢log⁡(𝒟⁢ℰ)⁢log⁡(U⁢V)8⁢log⁡x).M=\exp\!\left(\frac{9\log(\mathcal{D}\mathcal{E})\log(UV)}{8\log x}\right).

In this range 𝒟⁢ℰ>1\mathcal{D}\mathcal{E}>1, U⁢V>H1/2>1UV>H^{1/2}>1, and x>1x>1, so M>1M>1. If the sides are interchanged, the equation has h=−1h=-1. Reuss’s hypotheses are 1≤ℓ<k1\leq\ell<k, h≠0h\neq 0, log⁡(𝒟⁢ℰ)≍log⁡(U⁢V)≍log⁡x\log(\mathcal{D}\mathcal{E})\asymp\log(UV)\asymp\log x, and, when ℓ=1\ell=1, 𝒟⁢ℰ≫x1/k\mathcal{D}\mathcal{E}\gg x^{1/k}. We have 𝒟⁢ℰ≫H7/12≫x1/2\mathcal{D}\mathcal{E}\gg H^{7/12}\gg x^{1/2}, and the logarithmic comparabilities were established above. The estimate applies for large xx; bounded values of HH are absorbed in the implied constant. The resulting bound for the number NN in a cell is

(A.9) N\displaystyle N ≪εHε⁢min⁡{(𝒟⁢ℰ⁢M)1/2+𝒟+ℰ,(U⁢V⁢M)1/2+U+V},\displaystyle\ll_{\varepsilon}H^{\varepsilon}\min\left\{(\mathcal{D}\mathcal{E% }M)^{1/2}+\mathcal{D}+\mathcal{E},(UVM)^{1/2}+U+V\right\},
log⁡M\displaystyle\log M =9⁢log⁡(𝒟⁢ℰ)⁢log⁡(U⁢V)8⁢log⁡x.\displaystyle=\frac{9\log(\mathcal{D}\mathcal{E})\log(UV)}{8\log x}.

Write 𝒟⁢ℰ=Hθ\mathcal{D}\mathcal{E}=H^{\theta} up to constant factors. Since x≍Hx\asymp H and U⁢V≍H2/(𝒟⁢ℰ)2UV\asymp H^{2}/(\mathcal{D}\mathcal{E})^{2}, the determinant term in (A.9) has exponent at most

ϕ⁢(θ)+O⁢(1log⁡H),ϕ⁢(θ)=12⁢min⁡(θ,2−2⁢θ)+98⁢θ⁢(1−θ),712≤θ≤34.\phi(\theta)+O\left(\frac{1}{\log H}\right),\qquad\phi(\theta)=\frac{1}{2}\min% (\theta,2-2\theta)+\frac{9}{8}\theta(1-\theta),\quad\frac{7}{12}\leq\theta\leq% \frac{3}{4}.

The function increases up to θ=2/3\theta=2/3 and decreases afterwards, with

ϕ⁢(2/3)=13+14=712.\phi(2/3)=\frac{1}{3}+\frac{1}{4}=\frac{7}{12}.

It remains to bound the additive terms. For θ≤2/3\theta\leq 2/3, use the first branch of (A.9); by (A.6), 𝒟+ℰ≪H1/2\mathcal{D}+\mathcal{E}\ll H^{1/2}. For θ≥2/3\theta\geq 2/3, orient the cell so 𝒟≤ℰ\mathcal{D}\leq\mathcal{E}, hence U≥VU\geq V, and use the second branch. If U≤H7/12U\leq H^{7/12}, its additive term is already small enough. Otherwise U=x/𝒟2>H7/12U=x/\mathcal{D}^{2}>H^{7/12} gives 𝒟≪H5/24\mathcal{D}\ll H^{5/24}; together with 𝒟⁢ℰ≫H2/3\mathcal{D}\mathcal{E}\gg H^{2/3} this gives ℰ≫H11/24\mathcal{E}\gg H^{11/24} and V≪H1/12V\ll H^{1/12}. Fixing d,sd,s, the equation gives

f2⁢s≡1(modd2),f^{2}s\equiv 1\pmod{d^{2}},

or f2⁢s≡−1(modd2)f^{2}s\equiv-1\pmod{d^{2}} in the reversed orientation. Since (d,s)=1(d,s)=1, each sign has at most 4ω⁢(d)≪εHε4^{\omega(d)}\ll_{\varepsilon}H^{\varepsilon} roots modulo d2d^{2}. Counting ff in its interval for each root and summing over d≪𝒟d\ll\mathcal{D} and s≪Vs\ll V gives

N≪εHε⁢(ℰ⁢V𝒟+𝒟⁢V)≪εHε⁢(H𝒟⁢ℰ+𝒟⁢V)≪εH1/3+ε,N\ll_{\varepsilon}H^{\varepsilon}\left(\frac{\mathcal{E}V}{\mathcal{D}}+% \mathcal{D}V\right)\ll_{\varepsilon}H^{\varepsilon}\left(\frac{H}{\mathcal{D}% \mathcal{E}}+\mathcal{D}V\right)\ll_{\varepsilon}H^{1/3+\varepsilon},

since 𝒟⁢V≪H7/24\mathcal{D}V\ll H^{7/24}. Thus all additive terms are below H7/12+εH^{7/12+\varepsilon}. There are O⁢((log⁡H)2)O((\log H)^{2}) dyadic boxes and a bounded number of cells in each. Summing (A.8) and the bounds above over all cells, the logarithms are absorbed into HεH^{\varepsilon} and

(A.10) Nhi≪εH7/12+ε.N_{\mathrm{hi}}\ll_{\varepsilon}H^{7/12+\varepsilon}.

Combining (A.5) and (A.10) proves the theorem. ∎

Remark A.1.

Diao’s Lemma 2.1 [2] gives the 7/127/12 exponent for δ1⁢x12−δ2⁢x22=ϑ\delta_{1}x_{1}^{2}-\delta_{2}x_{2}^{2}=\vartheta in dyadic boxes with Δ1≤Δ2\Delta_{1}\leq\Delta_{2}, Δ1⁢Δ2≤B\Delta_{1}\Delta_{2}\leq B, and Δ1⁢X12=Δ2⁢X22=B\Delta_{1}X_{1}^{2}=\Delta_{2}X_{2}^{2}=B, where ϑ∈{±1,±2}\vartheta\in\{\pm 1,\pm 2\}. In our cell the scales are (Δ1,X1,Δ2,X2,B)=(V,ℰ,U,𝒟,x)(\Delta_{1},X_{1},\Delta_{2},X_{2},B)=(V,\mathcal{E},U,\mathcal{D},x), and the equation is s⁢f2−r⁢d2=1sf^{2}-rd^{2}=1. If the scales need to be ordered, interchanging the two sides changes ϑ\vartheta to −1-1. Since 𝒟⁢ℰ≫H7/12\mathcal{D}\mathcal{E}\gg H^{7/12} and x≍Hx\asymp H, U⁢V=x2/(𝒟⁢ℰ)2≪H5/6≪xUV=x^{2}/(\mathcal{D}\mathcal{E})^{2}\ll H^{5/6}\ll x for sufficiently large HH. Thus Diao’s condition Δ1⁢Δ2≤B\Delta_{1}\Delta_{2}\leq B holds. Diao proves Lemma 2.1 by combining the determinant estimate (2.1) with the Fouvry–Jouve estimate (2.2). The determinant input is the (k,ℓ)=(2,1)(k,\ell)=(2,1) case of Reuss’s Theorem 1 [9], applied above with h=±1h=\pm 1. Diao cites this estimate as Theorem 5 of Reuss’s 2015 thesis; his lemma therefore gives the high-product bound directly.

Use of AI tools

The author devised the main argument. Codex (OpenAI, GPT-6 Astra) carried out the numerical checks of the identities and of the cubic family and searched the literature. Claude Code (Anthropic, Claude Opus 5.5) checked the arguments and the references. The author checked every step of the proof and every reference, and takes full responsibility for the content of the paper.

Statements and declarations

Competing interests. The author has no competing interests.

Funding. No funding was received for this work.

Data availability. No data sets were generated or analyzed in this work.

References

  • [1] R. Balasubramanian, T. N. Shorey, and M. Waldschmidt, On the maximal length of two sequences of consecutive integers with the same prime divisors, Acta Math. Hungar. 54 (1989), no. 3–4, 225–236, https://doi.org/10.1007/BF01952052.
  • [2] Y. Diao, Class numbers and integer points on some Pellian surfaces, J. Théor. Nombres Bordeaux 37 (2025), no. 3, 973–988; https://doi.org/10.5802/jtnb.1348; arXiv:2408.03774v2 (2026).
  • [3] P. Erdős, How many pairs of products of consecutive integers have the same prime factors?, Amer. Math. Monthly 87 (1980), no. 5, 391–392, https://doi.org/10.1080/00029890.1980.11995045.
  • [4] P. Erdős and E. G. Straus, On products of consecutive integers, in: Number theory and algebra: collected papers dedicated to Henry B. Mann, Arnold E. Ross, and Olga Taussky-Todd, Academic Press, New York, 1977, 63–70.
  • [5] D. M. Kane, On a problem relating to the ABC conjecture, preprint (2011), arXiv:1104.2635v1.
  • [6] D. M. Kane, On the number of ABC solutions with restricted radical sizes, J. Number Theory 154 (2015), 32–43. https://doi.org/10.1016/j.jnt.2014.09.021; preprint version: arXiv:1104.2635v2 (2014). Proposition numbers refer to this version.
  • [7] N. Lebowitz-Lockard, On pairs of consecutive sequences with the same radicals, preprint (2025), arXiv:2507.09899v1.
  • [8] D. H. Lehmer, On a problem of Størmer, Illinois J. Math. 8 (1964), no. 1, 57–79, https://doi.org/10.1215/ijm/1256067456.
  • [9] T. Reuss, Pairs of kk-free numbers, consecutive square-full numbers, preprint (2014), arXiv:1212.3150v2.
  • [10] C. Sanna, On the exponents in the factorizations of rr consecutive numbers, Quaest. Math. 45 (2022), no. 8, 1221–1228. https://doi.org/10.2989/16073606.2021.1938277.
  • [11] T. Tao, Products of consecutive integers with unusual anatomy, preprint (2026), arXiv:2603.27990v3.