gpt pro 5.2 attempt on Math-927
mathematicsErdős problemscontributionManuscript
Contents
- Problem 768
- 1. Formal restatement
- Question (Erdős).
- 2. Quick literature/context check (web-browsing was available)
- 3. Strategy
- What would prove the conjectured asymptotic.
- What we can do unconditionally here.
- 4. Work
- 4.1 A density-$0$ theorem
- 4.2 Small-$N$ computational data
- 5. Obstacles/checks
- 6. Conclusion
- 7. If UNRESOLVED: what we have and what is missing
Problem 768
1. Formal restatement
- $d>1$, and
- $d\equiv 1\pmod p$.
For $N\ge 1$ define the counting function \[ A(N)\coloneqq |\{n\le N: n\in A\}|, \qquad \delta(N)\coloneqq \frac{A(N)}{N}. \]
Question (Erdős).
Is there a constant $c>0$ such that, as $N\to\infty$, \[ \delta(N)=\exp\left(-(c+o(1))\,\sqrt{\log N}\,\log\log N\right)? \] (Here and throughout, $\log$ is the natural logarithm.)2. Quick literature/context check (web-browsing was available)
The problem statement and its known bounds are recorded on the ErdosProblems project page for #768. The same set $A$ appears as OEIS A352287 ("Numbers surviving the Sylow test") and is discussed in a MathOverflow thread by M. Suárez-Álvarez (answer by W. Sawin) about the density of integers excluded by Sylow congruences for simple group orders.
A quick web search (Jan 2026) did not turn up a published proof of the conjectured sharp asymptotic with an explicit constant $c$.
3. Strategy
What would prove the conjectured asymptotic.
One needs an upper bound matching Erdős's lower bound of the shape $\delta(N)\le \exp(-(c'+o(1))\sqrt{\log N}\,\log\log N)$ for some constant $c'>0$ and in fact with $c'=c$. Heuristically, the bottleneck is controlling the constraint for the largest prime factor $P(n)$, because a divisor $\equiv 1\pmod{P(n)}$ must be of the form $1+aP(n)$, which forces substantial extra structure.What we can do unconditionally here.
We give a clean proof (following the idea in Sawin's MathOverflow answer) that $A$ has natural density $0$. This is far from the conjectured stretched-exponential asymptotic, but it is a rigorous "first barrier" result. We also provide small-$N$ computational data.4. Work
4.1 A density-$0$ theorem
Step 1: the "smooth" part can be made arbitrarily small. The set $S_\mathrm{smooth}(x)$ is contained in the set of $x^{\delta}$-smooth numbers. By standard estimates for smooth numbers (e.g. de Bruijn--Dickman asymptotics), for each $\varepsilon>0$ there exists a choice of $\delta>0$ such that for all sufficiently large $x$, \[ |S_\mathrm{smooth}(x)|\le \#\{n\le x: P(n)\le x^{\delta}\}\le \varepsilon x. \] (We will henceforth fix such a $\delta$ corresponding to an arbitrary small $\varepsilon$.)
Step 2: for fixed $\delta$, the "rough" part is $o(x)$. Let $n\in S_\mathrm{rough}(x)$ and put $p\coloneqq P(n)>x^{\delta}$. Because $n\in A$, applying the defining property to the prime $p\mid n$ yields a divisor $d\mid n$ with $d>1$ and $d\equiv 1\pmod p$. Write $d=1+ap$ with $a\ge 1$. Note that $p\nmid d$ (since $d\equiv 1\pmod p$), so we may write \[ n = p\,d\,b \] for some integer $b\ge 1$ (this absorbs the remaining prime-power factors of $n$, including possible additional factors of $p$). In particular, \[ n \ge p\,d = p(1+ap). \]
Now count such $n\le x$ by counting triples $(p,a,b)$. For fixed $p$ and $a$, the number of $b$ with $p(1+ap)b\le x$ is at most $x/(p(1+ap))$. Therefore \[ |S_\mathrm{rough}(x)| \le \sum_{\substack{p>x^{\delta}\\ p\text{ prime}}}\ \sum_{a\ge 1}\ \frac{x}{p(1+ap)}. \] For each prime $p$ we bound \[ \sum_{a\ge 1}\frac{1}{p(1+ap)} \le \frac{1}{p^2}\sum_{a\ge 1}\frac{1}{a} \quad\text{with the constraint } 1+ap\le x\ \text{ (else the summand contributes }0\text{).} \] More cleanly, since $1+ap\le x$ implies $a\le x/p$, we have \[ \sum_{1\le a\le x/p}\frac{1}{p(1+ap)} \le \frac{1}{p^2}\sum_{1\le a\le x/p}\frac{1}{a} \le \frac{\log x}{p^2} \] for all large $x$. Hence \[ |S_\mathrm{rough}(x)| \le x\log x\sum_{p>x^{\delta}}\frac{1}{p^2}. \] Using the crude bound $\sum_{m>y}m^{-2}\le 1/y$ we obtain \[ \sum_{p>x^{\delta}}\frac{1}{p^2}\le \sum_{m> x^{\delta}}\frac{1}{m^2}\le \frac{1}{x^{\delta}}. \] Therefore \[ |S_\mathrm{rough}(x)|\le x\log x\cdot x^{-\delta}=x^{1-\delta}\log x=o(x). \]
Step 3: conclude density $0$. Given any $\varepsilon>0$ choose $\delta$ as in Step 1. Then for sufficiently large $x$, \[ A(x)\le |S_\mathrm{smooth}(x)|+|S_\mathrm{rough}(x)|\le \varepsilon x + o(x). \] Dividing by $x$ and letting $x\to\infty$ gives $\limsup_{x\to\infty}A(x)/x\le \varepsilon$. Since $\varepsilon$ was arbitrary, $A(x)/x\to 0$. ∎
4.2 Small-$N$ computational data
A direct computation (trial division via smallest-prime-factor sieve, enumerating divisors of the $p$-free part for each prime $p\mid n$) gives:
- First few elements of $A$: \[ 1,12,24,30,36,48,56,60,72,80,90,96,105,108,112,120,\dots \]
- Densities: \[ \delta(10^4)=0.057,\qquad \delta(10^5)\approx 0.03276,\qquad \delta(2\cdot 10^5)\approx 0.02757,\qquad \delta(10^6)\approx 0.018462. \]
- The ratio $\displaystyle \frac{-\log\delta(N)}{\sqrt{\log N}\,\log\log N}$ for these $N$ is about $0.41$ (not remotely in an asymptotic regime, but consistent with a conjectural constant of that scale).
5. Obstacles/checks
The density-$0$ argument above is extremely lossy: it only uses one prime (the largest prime factor) and counts very crudely by the divisor form $1+ap$. To reach a sharp asymptotic of the form $\exp(-(c+o(1))\sqrt{\log N}\,\log\log N)$ one would need:
- a much finer understanding of the typical size of the largest prime factor $P(n)$ among $n\in A$;
- a sieve analysis of how often $n$ can contain, simultaneously for many primes $p\mid n$, a nontrivial divisor $\equiv 1\pmod p$;
- matching upper and lower bounds on a stretched-exponential scale.
6. Conclusion
UNRESOLVED. The conjectured sharp asymptotic with constant $c$ remains open (as far as found in the quick literature check). What is proved here is that $A$ has density $0$, and we provide small computational data.
7. If UNRESOLVED: what we have and what is missing
- Strongest proved statement here: $A(N)=o(N)$ (density $0$), with an explicit upper bound of the form $A(x)\ll x^{1-\delta}\log x + \Psi(x,x^{\delta})$ for any fixed small $\delta>0$.
- First genuine gap toward the conjecture: proving an upper bound of the correct stretched-exponential order $\exp(-c\sqrt{\log N}\,\log\log N)$, rather than just $o(1)$ density.
- A plausible route: sharpen the "largest prime factor" counting to the regime $p\approx \exp(\sqrt{\log N\log\log N})$ and combine with de Bruijn asymptotics for smooth numbers; then analyze additional constraints from smaller prime factors.