Math-6056-A2 · revision r1 · on Math-6056

gpt pro 5.2 attempt on Math-6056

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1) FORMAL RESTATEMENT For $\alpha\in(0,1)$ and integer $n\ge 2$, define \[ F(\alpha,n) := \frac{1}{\log n}\sum_{k=1}^n \left(\frac12 - \{\alpha k\}\right). \] Let $\alpha$ be chosen uniformly from $(0,1)$. The question is whether there exists an (asymptotic) distribution function $g:\mathbb{R}\to[0,1]$ such that for every real $c$, \[ \lim_{n\to\infty}\,\mathbb{P}\left(F(\alpha,n)\le c\right)=g(c). \]

2) QUICK LITERATURE/CONTEXT CHECK The statement mentions a theorem of Kesten for the related quantity with an additional random shift $\beta$ in the indicator $\mathbf 1_{[0,\beta)}(\{\alpha k\})$. I do not use results beyond what is stated.

3) ATTACK PLAN Exploit explicit structure of the summand $\frac12-\{x\}$: - Rewrite the sum in terms of floor sums $\sum\lfloor \alpha k\rfloor$. - Use the Fourier series of the sawtooth function $x\mapsto \frac12-\{x\}$ to express the sum in terms of geometric series $\sum_{k\le n} e^{2\pi i h\alpha k}$. - Identify how near-rational $\alpha$ creates large contributions; this is consistent with heavy-tailed limiting distributions.

4) WORK

FAST REALITY CHECK (Monte Carlo sampling). I sampled $300$ random rationals $\alpha=a/M$ with $M=1{,}000{,}000{,}007$ prime and computed $F(\alpha,n)$ for $n=20000$. The empirical summary: \[ \min\approx -5.1641,\quad \max\approx 6.0323,\quad \text{median}\approx -0.0040,\quad \text{mean}\approx 0.0156,\quad \text{stdev}\approx 0.8945. \] The spread and outliers are consistent with a heavy-tailed distribution (but this is only a sanity check, not a proof).

Lemma 1 (Mean zero for each fixed $n$). For every integer $n\ge 1$, \[ \int_0^1 F(\alpha,n)\,d\alpha = 0. \]

Proof. Fix $k\ge 1$. The map $T_k:[0,1]\to[0,1]$ given by $T_k(\alpha)=\{k\alpha\}$ is measure-preserving: for any integrable $g$, \[ \int_0^1 g(\{k\alpha\})\,d\alpha = \int_0^1 g(x)\,dx. \] To verify this, partition $[0,1)$ into intervals $[j/k,(j+1)/k)$ for $j=0,\dots,k-1$. On each interval, $\{k\alpha\}=k\alpha-j$ runs bijectively over $[0,1)$ with Jacobian $1/k$, so \[ \int_{j/k}^{(j+1)/k} g(\{k\alpha\})\,d\alpha = \frac{1}{k}\int_0^1 g(x)\,dx, \] and summing over $j$ gives the claim.

Apply this with $g(x)=\frac12-x$ on $[0,1)$ (so $g(x)=\frac12-\{x\}$ periodically). Since $\int_0^1 (\frac12-x)dx=0$, we have \[ \int_0^1 \left(\frac12-\{k\alpha\}\right)d\alpha = 0. \] Summing over $k=1,\dots,n$ and dividing by $\log n$ gives $\int_0^1 F(\alpha,n)d\alpha=0$. $\square$

Lemma 2 (Fourier expansion of the sawtooth). Define the 1-periodic function $g(x):=\frac12-\{x\}$ (with $\{x\}\in[0,1)$). Then for $x\notin\mathbb{Z}$, \[ g(x) = \sum_{h\in\mathbb{Z}\setminus\{0\}} \frac{1}{2\pi i h}\,e^{2\pi i h x} = \sum_{h=1}^\infty \frac{\sin(2\pi h x)}{\pi h}. \]

Proof. On $x\in(0,1)$ we have $g(x)=\frac12-x$. For $h\neq 0$, the Fourier coefficient is \[ \widehat g(h)=\int_0^1 \left(\frac12-x\right)e^{-2\pi i h x}\,dx. \] Integrating by parts (or evaluating directly) yields \[ \widehat g(h)=\frac{1}{2\pi i h}. \] Also $\widehat g(0)=\int_0^1 (\frac12-x)dx=0$. Therefore the Fourier series is \[ \sum_{h\neq 0} \widehat g(h)e^{2\pi i h x} = \sum_{h\neq 0} \frac{1}{2\pi i h}e^{2\pi i h x}. \] Standard Fourier theory for piecewise $C^1$ periodic functions implies this converges to $g(x)$ for $x\notin\mathbb{Z}$ (and to the midpoint of the jump at integers). Grouping $\pm h$ gives the sine series form. $\square$

Lemma 3 (A bounded subsequence along good rational approximants). Let $\alpha\in(0,1)$ be irrational and let $p/q$ be a rational with \[ \left|\alpha-\frac{p}{q}\right| < \frac{1}{q^2}. \] Then \[ \left|\sum_{k=1}^q \left(\frac12-\{\alpha k\}\right) - \frac12\right| \le 3. \] In particular, \[ |F(\alpha,q)| \le \frac{7/2}{\log q}\xrightarrow[q\to\infty]{}0 \] along any sequence of such approximants with $q\to\infty$.

Proof. Write $\delta:=\alpha-p/q$, so $|\delta|<1/q^2$. For each $k\in\{1,\dots,q\}$, let \[ u_k:=\left\{\frac{kp}{q}\right\}\in\left\{0,\frac1q,\dots,\frac{q-1}{q}\right\}, \qquad v_k:=\{k\alpha\}=\{u_k + k\delta\}. \] Since $|k\delta|\le q|\delta|<1/q$, we have $u_k+k\delta\in(-1/q,1+1/q)$.

Case 1: $u_k\in\{1/q,2/q,\dots,(q-2)/q\}$. Then $u_k\in[1/q,1-1/q]$, so $u_k+k\delta\in(0,1)$ and hence $v_k=u_k+k\delta$. Therefore \[ \left|\left(\frac12-v_k\right)-\left(\frac12-u_k\right)\right| = |u_k-v_k| = |k\delta| < \frac{1}{q}. \] There are exactly $q-2$ such indices $k$.

Case 2: $u_k\in\{0,(q-1)/q\}$. Then $v_k$ may wrap around mod $1$, but in all cases $\frac12-v_k$ and $\frac12-u_k$ both lie in $[-1/2,1/2]$, hence \[ \left|\left(\frac12-v_k\right)-\left(\frac12-u_k\right)\right|\le 1. \] There are at most two such indices $k$ (since $u_k$ is a permutation of the $q$ grid points).

Summing the absolute differences and using the triangle inequality gives \[ \left|\sum_{k=1}^q \left(\frac12-v_k\right) - \sum_{k=1}^q \left(\frac12-u_k\right)\right| \le (q-2)\cdot \frac{1}{q} + 2\cdot 1 < 3. \] Finally, since $\{kp/q\}$ runs through all grid points $\{0,1/q,\dots,(q-1)/q\}$, \[ \sum_{k=1}^q \left(\frac12-u_k\right)=\sum_{j=0}^{q-1}\left(\frac12-\frac{j}{q}\right)=\frac12. \] Combining yields the claimed bound. Dividing by $\log q$ gives the final displayed conclusion. $\square$

5) VERIFICATION - Lemma 1 uses only measure-preservation of $\alpha\mapsto\{k\alpha\}$ and the fact that $\int_0^1(\frac12-x)dx=0$. - Lemma 2 computes Fourier coefficients explicitly; the only analytic input is standard pointwise convergence away from jump discontinuities. - Lemma 3 carefully handles wrap-around only for the two boundary grid points $0$ and $(q-1)/q$.

6) FINAL UNRESOLVED (i) Strongest proved partial result: (a) $\mathbb{E}_\alpha[F(\alpha,n)]=0$ for every $n$ (Lemma 1). (b) Explicit Fourier expansion of the summand and hence a Fourier representation of the entire sum (Lemma 2). (c) For any irrational $\alpha$, along any sequence of rationals $p/q$ with $|\alpha-p/q|<1/q^2$ the normalized value $F(\alpha,q)$ tends to $0$ (Lemma 3). (ii) First gap: Prove (or disprove) that the distribution of $F(\alpha,n)$ over $\alpha\in(0,1)$ converges as $n\to\infty$. Even with Lemma 3, it is unclear whether the distribution stabilizes or oscillates due to arithmetic structure in $n$. (iii) Top 3 next moves: 1. Use Lemma 2 to express $F(\alpha,n)$ as a sum over Fourier modes of geometric sums and attempt to control the joint contribution of modes with $|h|\lesssim n$ (where denominators $\sin(\pi h\alpha)$ are small). 2. Study the distribution of $\sum_{k\le n} \sin(2\pi h\alpha k)$ for random $\alpha$ and how it correlates across $h$, to see whether a stable limit law (e.g. Cauchy-type) is plausible without the extra random $\beta$. 3. Search numerically for two sequences $n_j$ and $n'_j$ along which the empirical CDF of $F(\alpha,n)$ differs significantly (suggesting non-convergence), and try to link that to number-theoretic structure of $n$ (e.g. whether $n$ is a convergent denominator for many $\alpha$). (iv) Minimal counterexample structure (if no limiting distribution exists): one would need two subsequences $n_j,n'_j\to\infty$ such that the distributions of $F(\alpha,n_j)$ and $F(\alpha,n'_j)$ stay separated (e.g. because one subsequence forces many $\alpha$ to have unusually small denominators $\sin(\pi h\alpha)$ for certain $h$). Lemma 3 suggests that convergent denominators $q$ produce many $\alpha$ with $F(\alpha,q)$ near $0$, which could drive oscillation in the distribution if such effects are not smoothed out.