Cut the unit circle at the fractional parts {1},…,{N}\{\sqrt{1}\},\dots,\{\sqrt{N}\}; the complementary intervals (gaps), normalized by the mean gap 1/N1/N, have a limiting distribution that is not exponential, by the theorem of Elkies and McMullen (Duke Math. J. 2004), proved via Ratner's theorem on the space of affine unimodular lattices. Their paper asked for effective and explicit versions of this result: error terms for the convergence, closed-form formulas for the truncated-window density F(θ)(t)F^{(\theta)}(t) and for the dilated densities Fu(θ)(t)F_u^{(\theta)}(t) when u∈Qu\in\mathbb{Q} and 2/u∉Z2/u\notin\mathbb{Z}, explicit joint distributions of consecutive gaps, and the conjectural exponential (Poisson) gap law for {un}\{\sqrt{un}\} with irrational uu. Subsequent literature has made the convergence effective for the base sequence (Strömbergsson 2015; Browning and Vinogradov 2016; Vinogradov 2016) and produced a new circle-method proof (Radziwiłł and Technau 2024), while Poissonian pair correlation was proved by El-Baz, Marklof and Vinogradov (2015) and pigeonhole statistics by Pattison. The effective-rates question is now largely resolved, but a precise, nonempty open core survives: the explicit formulas, the structure of the multi-gap joint laws, and the irrational-dilation exponential law.

Background

For a real number xx, write {x}=x mod 1\{x\}=x\bmod 1 for its fractional part in R/Z\mathbb{R}/\mathbb{Z}. A classical theme of uniform distribution theory asks how evenly such sequences fill the circle; a sharper question is their fine-scale statistics, for which the lengths of the gaps between consecutive points are a standard probe. If NN points are placed independently and uniformly at random, the gaps JJ normalized by the mean gap 1/N1/N obey the exponential law #J:∣J∣∈[a/N,b/N]/N→∫abe−t dt\#{J:|J|\in[a/N,b/N]}/N\to\int_a^b e^{-t}\,dt, the gap law of a Poisson process; observing this law is regarded as evidence of pseudo-randomness.

Elkies and McMullen studied the gaps J1,…,JNJ_1,\dots,J_N left when the circle is cut at {1},…,{N}\{\sqrt{1}\},\dots,\{\sqrt{N}\}. Their main theorem (Theorem 1.1) states that N∣Ji∣N|J_i| is governed in the limit by a piecewise real-analytic density F(t)F(t) with genuine phase transitions at t=1/2t=1/2 and t=2t=2: FF is constant (equal to 6/π26/\pi^2) on [0,1/2][0,1/2] and has a power-law tail F(t)∼(3/π2)t−3F(t)\sim(3/\pi^2)t^{-3} rather than an exponential one. Thus {n}\{\sqrt{n}\} is conspicuously non-Poissonian at the level of gaps, in contrast to the conjectural exponential behavior of {nβ}\{n^{\beta}\} for β∈(0,1)\beta\in(0,1), β≠1/2\beta\neq 1/2.

The proof connects the gap problem to homogeneous dynamics. A unimodular lattice in R2\mathbb{R}^2 is a discrete subgroup isomorphic to Z2\mathbb{Z}^2 with quotient torus of area one; a lattice translate is a coset v+Λ0v+\Lambda_0. The space of all such translates is the homogeneous space E=ASL2(R)/ASL2(Z)E=\mathrm{ASL}_2(\mathbb{R})/\mathrm{ASL}_2(\mathbb{Z}) of dimension 5, where ASL2\mathrm{ASL}_2 denotes area-preserving affine maps; EE carries a unique invariant probability measure μE\mu_E. Elkies and McMullen show that the gap containing a random point x∈[0,1]x\in[0,1] is controlled by a lattice translate Λs2(x)\Lambda_{s^2}(x) obtained by a linearization of (a+x)2(a+x)^2, and that the family Λs2(x)\Lambda_{s^2}(x) equidistributes in EE (their Theorem 1.2), a consequence of Ratner's theorem classifying measures invariant under unipotent flows (a unipotent flow is the action of a one-parameter subgroup of unipotent, i.e. parabolic, matrices such as (1t01)\begin{pmatrix}1&t\\0&1\end{pmatrix}; the Λs2(x)\Lambda_{s^2}(x) traverse a nonlinear horocycle section, i.e. a curve whose projection to SL2(R)/SL2(Z)\mathrm{SL}_2(\mathbb{R})/\mathrm{SL}_2(\mathbb{Z}) is a closed horocycle, a circle of large period). Consequently, if p(t)p(t) denotes the probability that a random lattice translate meets a fixed triangle of area tt, then p′′(t)=−F(t)p''(t)=-F(t); the paper evaluates this to an explicit elementary formula for FF (involving arctangents and logarithms, its Theorem 3.14).

Two generalizations frame the open questions. First, restricting the indices to the truncated window θ2N<n≤N\theta^2N<n\le N (0<θ<10<\theta<1; the window then contains (1−θ2)N+O(1)(1-\theta^2)N+O(1) points, and the gaps are still measured in units of 1/N1/N, the number of gaps with length in [t0/N,t1/N][t_0/N,t_1/N] being asymptotic to N∫t0t1F(θ)(t) dtN\int_{t_0}^{t_1}F^{(\theta)}(t)\,dt) replaces the governing triangle by an isosceles trapezoid and yields a modified gap density F(θ)(t)F^{(\theta)}(t), for which the paper obtains only a double-integral representation (its Theorem 3.15): F(θ)F^{(\theta)} is piecewise analytic, constant equal to (1−θ2)2/ζ(2)(1-\theta^2)^2/\zeta(2) on [0,1/(2−2θ)][0,1/(2-2\theta)] (here ζ(2)=∑n≥1n−2=π2/6\zeta(2)=\sum_{n\ge1}n^{-2}=\pi^2/6 is the Riemann zeta function at 22), and has a t−3t^{-3} tail. Second, fixing a rational u>0u>0 and real ν\nu, one may take the gaps of {un+ν}\{\sqrt{un+\nu}\} with 0<un+ν<N0<un+\nu<N; the gap law, with gaps measured in units of u/Nu/N (the proportion of gaps with length in [t0u/N,t1u/N][t_0u/N,t_1u/N] tends to ∫t0t1Fu(t) dt\int_{t_0}^{t_1}F_u(t)\,dt), converges to a limit Fu(t)F_u(t) independent of ν\nu but depending on uu, constructed from the periodic set ω1/uZ2\omega_{1/u}\mathbb{Z}^2, where ωv(x,y)=(x,y+v2x)\omega_v(x,y)=(x,y+v^2x). Writing u=u1/u2u=u_1/u_2 in lowest terms, ω1/uZ2\omega_{1/u}\mathbb{Z}^2 is a disjoint union of at most u1u_1 translates of a lattice and is itself a lattice translate only when u1∣2u_1\mid 2; the corresponding moduli space is E(u)=ASL2(R)/Γ(u)E(u)=\mathrm{ASL}_2(\mathbb{R})/\Gamma(u), where Γ(u)\Gamma(u) is the stabilizer of ω1/uZ2\omega_{1/u}\mathbb{Z}^2 in ASL2(R)\mathrm{ASL}_2(\mathbb{R}), a congruence subgroup containing the 3×33\times3 matrices in ASL2(Z)\mathrm{ASL}_2(\mathbb{Z}) congruent to the identity modulo u1u_1. Elementary closed forms are available only in the lattice case (2/u∈Z2/u\in\mathbb{Z}); beyond the general existence theorem, Elkies and McMullen prove that Fu(0)<1F_u(0)<1 for all uu, that Fu(0)→1F_u(0)\to 1 as u1→∞u_1\to\infty, and give an orbit-sum formula for Fu(0)F_u(0) when u1=pu_1=p or 2p2p for an odd prime pp. Finally, the joint distribution of rr consecutive normalized gaps converges by the same method to a law supported on a countable union of manifolds of dimension at most 5=dim⁡E5=\dim E, whose part inside the simplex ∑jtj<1/2\sum_j t_j<1/2 has dimension exactly 2 (it comes from collinear lattice points and is therefore singular once r>2r>2); with the truncated window the simplex becomes ∑jtj<1/(2−2θ)\sum_j t_j<1/(2-2\theta).

Subsequent literature has developed the effective side of this theory: Strömbergsson (2015) and Browning and Vinogradov (2016) made the equidistribution of horocycle sections effective, the latter obtaining the quantitative gap-distribution error ∣λN(t)−λ∞(t)∣≪ε(1/t2+t)N−1/68+ε|\lambda_N(t)-\lambda_\infty(t)|\ll_\varepsilon(1/t^2+t)N^{-1/68+\varepsilon}, and Vinogradov (2016) treated general horocycle lifts; Strömbergsson, Södergren and Vishe (2026) generalized the effective equidistribution to SL2(R)⋉(R2)k\mathrm{SL}_2(\mathbb{R})\ltimes(\mathbb{R}^2)^k. Radziwiłł and Technau (2024) gave an essentially self-contained proof of the gap theorem by the circle method (a technique of analytic number theory that rewrites the relevant counting function as an integral over the unit circle, estimated separately on arcs near roots of unity and on the remaining arcs). Complementary fine-scale statistics were computed by El-Baz, Marklof and Vinogradov (2015), who proved that the two-point correlation function of {n}\{\sqrt{n}\} (the asymptotic density of pairs of points at a given small separation, scaled by the mean spacing) is Poissonian, and by Pattison (2023), who determined the pigeonhole statistics (the limit of the number of points of {n}\{\sqrt{n}\} falling in each of NN equal intervals). None of these addresses the explicit formulas for F(θ)F^{(\theta)} and FuF_u, the multi-gap joint laws, or the irrational-dilation regime.

Problem Statement

The common objective is to replace the qualitative existence theorems of Elkies and McMullen for the gap statistics of {un}\{\sqrt{un}\} by effective, explicit, and dilation-uniform descriptions. The problem is the surviving open core of their Section 3.6 'Open questions', with the rates component already substantially resolved by later work (see Background) and only its residue retained. A solution settles the following linked components; the first three constitute the core, and each asks for proofs, not numerical evidence alone.

(1) Explicit formulas. Determine whether the truncated-window gap density F(θ)(t)F^{(\theta)}(t), which governs the normalized gaps of {n}\{\sqrt{n}\} restricted to θ2N<n<N\theta^2N<n<N, is expressible as an elementary function of tt and θ\theta, and if so, give the formula. Answer the same question for Fu(θ)(t)F_u^{(\theta)}(t) for rational u>0u>0 with 2/u∉Z2/u\notin\mathbb{Z}, the case not covered by the elementary formulas available when 2/u∈Z2/u\in\mathbb{Z} (here Fu(θ)F_u^{(\theta)} is defined by the Elkies-McMullen construction via the periodic set ω1/uZ2\omega_{1/u}\mathbb{Z}^2 and the moduli space E(u)E(u)).

(2) Joint distributions. Determine whether the joint distribution of r>1r>1 consecutive normalized gaps of {un}\{\sqrt{un}\} (including the θ\theta-truncated and rational-uu variants) can be obtained explicitly for any r>1r>1; if not, at least locate the phase transitions and the supports of these joint distributions on [0,∞)r[0,\infty)^r: identify which manifolds carry positive mass, and determine their dimensions, so as to sharpen the paper's bounds (support in manifolds of dimension at most 5; dimension exactly 2 inside the simplex ∑jtj<1/2\sum_j t_j<1/2, or ∑jtj<1/(2−2θ)\sum_j t_j<1/(2-2\theta) for the truncated window).

(3) Irrational dilation. For irrational u>0u>0: does Fui(t)→e−tF_{u_i}(t)\to e^{-t} for each fixed t≥0t\ge 0 whenever uiu_i are rationals approaching uu (the source paper notes this is known only for u=0u=0)? Prove or refute the conjecture, suggested by numerical experiments, that the normalized gaps of {un}\{\sqrt{un}\} converge to the exponential (Poisson) gap law for fixed irrational uu - in full (over all N→∞N\to\infty) for some explicit class of irrational uu, and also for almost all irrational uu; and answer the same questions for the truncated-window densities Fu(θ)F_u^{(\theta)} and for the joint distributions of consecutive gaps.

(4) Residue of the rates question (secondary). Improve the effective convergence rate of the gap-counting functions beyond the known N−1/68+εN^{-1/68+\varepsilon} error, and determine which of the two error sources - the linear approximation of (a+t)2(a+t)^2 or the rate of equidistribution of the horocycle sections Λs2(x)\Lambda_{s^2}(x) - accounts for the observed finite-NN behavior at normalized gap sizes below 1/21/2.

References

  1. Noam D. Elkies and Curtis T. McMullen, 'Gaps in n\sqrt{n} mod 1 and ergodic theory', Duke Mathematical Journal 123 (2004), no. 1, 95-139, DOI 10.1215/s0012-7094-04-12314-0, https://doi.org/10.1215/s0012-7094-04-12314-0 (published version also openly available via the Harvard DASH persistent handle https://dash.harvard.edu/handle/1/3637161, direct bitstream https://dash.harvard.edu/bitstream/1/3637161/5/McMullen_GapsErgodoticTheory.pdf; Section 3.6, 'Open questions', of this paper poses the questions set out in the Problem Statement)
  2. Noam D. Elkies and Curtis T. McMullen, 'Correction to Gaps in n\sqrt{n} mod 1 and ergodic theory', Duke Mathematical Journal 129 (2005), no. 2, DOI 10.1215/s0012-7094-05-12927-1, https://doi.org/10.1215/s0012-7094-05-12927-1
  3. Andreas Strömbergsson, 'An effective Ratner equidistribution result for SL(2,R)⋉R2\mathrm{SL}(2,\mathbb{R})\ltimes\mathbb{R}^2', Duke Mathematical Journal 164 (2015), no. 5, 843-902, DOI 10.1215/00127094-2885873, https://doi.org/10.1215/00127094-2885873 (preprint arXiv:1309.6103, https://arxiv.org/abs/1309.6103, posted under the variant title 'An Effective Ratner Equidistribution Result for ASL(2,R)')
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