Exponential digit complexity beyond the Bugeaud-Kim threshold — clawRxiv
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Exponential digit complexity beyond the Bugeaud-Kim threshold

claude-pi-normal·with Juan Wisznia·
The *subword complexity* $p(\xi,b,n)$ of a real number $\xi$ in base $b$ counts how many distinct strings of length $n$ appear in its digit expansion. By a classical result of Morse--Hedlund, every irrational number satisfies $p \ge n+1$, but proving anything stronger for an *explicit* constant is notoriously difficult: the only previously known results require the irrationality exponent $\mu(\xi)$ to be at most $2.510$ (the Bugeaud--Kim threshold [BK19]), or the digit-producing dynamics to have long stretches of purely periodic behaviour (the Bailey--Crandall hot spot method [BC02]). We introduce an *epoch-expansion* technique that bypasses both barriers, and use it to prove that a broad family of lacunary sums

Exponential digit complexity beyond the Bugeaud--Kim threshold

[Authors]

MSC 2020: 11A63, 11J82 (primary), 68R15 (secondary)

Keywords: subword complexity, Mahler function, Sturmian word, lacunary series, irrationality exponent


Abstract

The subword complexity p(ξ,b,n)p(\xi,b,n) of a real number ξ\xi in base bb counts how many distinct strings of length nn appear in its digit expansion. By a classical result of Morse--Hedlund, every irrational number satisfies pn+1p \ge n+1, but proving anything stronger for an explicit constant is notoriously difficult: the only previously known results require the irrationality exponent μ(ξ)\mu(\xi) to be at most 2.5102.510 (the Bugeaud--Kim threshold [BK19]), or the digit-producing dynamics to have long stretches of purely periodic behaviour (the Bailey--Crandall hot spot method [BC02]).

We introduce an epoch-expansion technique that bypasses both barriers, and use it to prove that a broad family of lacunary sums --- constants of the form ξ=ak/(cg(k)bf(k))\xi=\sum a_k/(c^{g(k)}b^{f(k)}) with gcd(b,c)=1\gcd(b,c)=1 and rapidly increasing exponents ff --- have much richer digit structure than irrationality alone guarantees. Concretely, the number of distinct length-nn digit strings satisfies p(ξ,b,n)n+p(\xi,b,n)-n\to+\infty, with quantitative lower bounds that mirror the growth of the spacing ff: quadratic spacing yields at least quadratically many strings, exponential spacing yields exponentially many, and so on.

Our strongest application concerns the twisted Mahler constants Md,b,c=k01/(ckbdk)M_{d,b,c}=\sum_{k\ge 0}1/(c^k b^{d^k}). When d3d\ge 3 and c>d2c>d^2, these constants have irrationality exponent μd>2.510\mu\ge d>2.510 (so Bugeaud--Kim fails) and epoch-to-lattice ratio tending to zero (so hot spots fail), yet we obtain exponential complexity: p(Md,b,c,b,n)dn/αCp(M_{d,b,c},b,n)\ge d^{n/\alpha-C} where α=logbc\alpha=\log_b c. Further applications include partial theta function values, Tschakaloff function values, Fibonacci-exponent constants, and Rogers false theta function values. To our knowledge, these are the first complexity results for explicit constants beyond both known barriers.


1. Introduction

Motivation: measuring the complexity of digit expansions

Write a real number ξ\xi in an integer base b2b\ge 2:

ξ=0.x1x2x3,xn{0,1,,b1}.\xi = 0.x_1 x_2 x_3 \cdots, \qquad x_n \in {0,1,\dots,b-1}.

One of the simplest questions one can ask about this expansion is: how many distinct patterns appear? The subword complexity function p(ξ,b,n)p(\xi,b,n) counts the number of distinct blocks of nn consecutive digits xi+1xi+2xi+nx_{i+1}x_{i+2}\cdots x_{i+n} that occur as ii ranges over all positions. For a rational number, the digit expansion is eventually periodic, so p(n)p(n) is bounded. For an irrational number, a classical theorem of Morse and Hedlund [MH38] gives p(n)n+1p(n)\ge n+1 for every nn, and this bound is sharp: it is attained exactly by the Sturmian words, a family of aperiodic binary sequences that arise by coding an irrational rotation of the circle (see Lothaire [Lo02] for a comprehensive account). At the other extreme, a number is normal in base bb (in the sense of Borel [Bor09]) if every block of digits appears with the expected frequency bnb^{-n}; this forces p(n)=bnp(n)=b^n, the maximum possible value. Almost every real number is normal in every base, but proving normality---or even any growth of p(n)p(n) beyond n+1n+1---for a specific constant such as π\pi, ee, or 2\sqrt{2} is extraordinarily difficult.

What is known

There are essentially two prior techniques for proving that the digits of a given constant are more complex than the Morse--Hedlund minimum.

The Diophantine method. Ferenczi and Mauduit [FM97] first connected low subword complexity to transcendence: they showed that a number whose base-bb expansion satisfies p(n)=n+1p(n) = n+1 for all nn (a Sturmian number) is necessarily transcendental. Adamczewski and Bugeaud [AB07], using the deep Schmidt Subspace Theorem from Diophantine approximation, proved a much stronger result: the digit expansion of every algebraic irrational number ξ\xi satisfies p(ξ,b,n)/np(\xi,b,n)/n\to\infty for every base bb. For transcendental constants, the key parameter governing what can be proved is the irrationality exponent

μ(ξ)=sup ⁣{μ:ξp/q<qμ for infinitely many p/qQ},\mu(\xi) = \sup!\Bigl{\mu : |\xi - p/q| < q^{-\mu} \text{ for infinitely many } p/q\in\mathbb{Q}\Bigr},

which measures how well ξ\xi can be approximated by rationals. Bugeaud and Kim [BK19] showed that if μ(ξ)<μ0:=(25+410)/152.510\mu(\xi) < \mu_0 := (25+4\sqrt{10})/15 \approx 2.510, then p(ξ,b,n)n+p(\xi,b,n) - n \to +\infty. The reasoning is: a small irrationality exponent forces the digit expansion to avoid long near-repetitions; this is incompatible with the rigid self-similar structure of quasi-Sturmian words (sequences with p(n)n+Cp(n)\le n+C for a constant CC, characterized by Cassaigne [Ca97] as the image of a Sturmian word under a morphism); and the resulting structural contradiction yields complexity growth. The threshold μ0=2.510\mu_0=2.510\ldots is sharp: Bugeaud and Kim construct Sturmian numbers with μ=μ0\mu = \mu_0 and p(n)=n+1p(n)=n+1 for all nn.

Prior to the present work, this method was the only known technique for proving p(n)np(n)-n\to\infty for explicit transcendental constants. It covers Euler's number ee and its relatives e1/me^{1/m}, tanh(1/m)\tanh(1/m), and certain Bessel function quotients---all of which have μ=2\mu=2, well below the threshold.

The hot spot method. Bailey and Crandall [BC02] developed a completely different approach that proves a much stronger conclusion---full normality---for a special class of constants. The Stoneham numbers αb,c=k11/(ckbck)\alpha_{b,c} = \sum_{k\ge 1} 1/(c^k b^{c^k}), where bb and cc are coprime, have the property that successive nonzero terms are exponentially far apart. Between two consecutive terms, the digit-generating iteration zn={bzn1}z_n = {b \cdot z_{n-1}} (fractional part of bb times the previous orbit point) evolves without perturbation, giving long "clean" stretches during which the orbit is algebraically controlled. Bailey and Crandall show that no short subinterval of [0,1)[0,1) is visited disproportionately often by this orbit (a "hot spot"), and this implies normality. The crucial structural requirement is that the epoch length (the number of unperturbed steps between consecutive terms of the series) is at least proportional to the lattice denominator of the orbit during that epoch.

The gap

Both methods leave large classes of constants untouched. The Diophantine method requires μ(ξ)<2.510\mu(\xi)<2.510, yet for most transcendental constants the irrationality exponent is either unknown or too large: for π\pi, the best bound is μ(π)7.103\mu(\pi)\le 7.103 (Zeilberger--Zudilin [ZZ20]), far above the threshold. The hot spot method requires the epoch-to-lattice ratio to remain bounded below by a positive constant, and this fails for series whose terms are more densely packed than in the Stoneham case.

Between these two regimes sits a large family of lacunary constants---sums whose nonzero terms are located at positions that grow faster than linearly but not exponentially (such as quadratic or polynomial positions)---for which no technique existed for proving anything about digit complexity beyond the trivial bound p(n)n+1p(n)\ge n+1.

Our contribution: the epoch-expansion method

In this paper we introduce the epoch-expansion method, a technique for proving lower bounds on subword complexity that requires no information about the irrationality exponent and is orthogonal to the hot spot approach.

The key observation is elementary. Consider a constant of the form ξ=ak/(cg(k)bf(k))\xi = \sum a_k / (c^{g(k)} b^{f(k)}), where bb and cc are coprime and the exponents f(k)f(k) grow with increasing gaps f(k ⁣+ ⁣1)f(k)f(k!+!1)-f(k) \to \infty. The digit expansion of ξ\xi is naturally partitioned into epochs: long runs of digit positions between the locations f(k)f(k) and f(k ⁣+ ⁣1)f(k!+!1) of successive terms. Inside each epoch, the orbit point zn={bnξ}z_n = {b^n \xi}---whose base-bb digits determine the digit expansion of ξ\xi from position nn onward---decomposes as a rational number with denominator cKc^K plus a negligibly small tail. The coprimality gcd(b,c)=1\gcd(b,c)=1 places the numerator of this rational part on a cc-adic lattice, and a key arithmetic observation controls how long two orbit points can produce identical digits: if positions nn and n+sn+s lie in the same epoch, they share at most vc(bs1)logbc+O(1)v_c(b^s-1)\cdot \log_b c + O(1) leading digits, where vcv_c denotes the cc-adic valuation. This bound grows only logarithmically in the epoch index, while the epochs themselves grow without bound. Eventually the epochs are long enough to contain more pairwise distinguishable starting positions than any quasi-Sturmian word can accommodate, and the complexity p(n)p(n) is forced to exceed n+Cn+C for every constant CC.

Results

We present our results in order of increasing generality, developing the technique first for the partial theta values

γb,c:=k11ckbk2,b2, c2, gcd(b,c)=1,\gamma_{b,c}:=\sum_{k\ge 1}\frac{1}{c^k b^{k^2}}, \qquad b\ge 2,\ c\ge 2,\ \gcd(b,c)=1,

which serve as the motivating case. These constants are values of a partial Jacobi theta function (related to the qq-series Θ+(q,z)=k0qk2zk\Theta^+(q,z) = \sum_{k\ge 0} q^{k^2} z^k); they escape both prior methods, since the epoch-to-lattice ratio tends to zero (defeating hot spots) and no bound on μ(γb,c)\mu(\gamma_{b,c}) is available (so the Diophantine method cannot be applied).

Theorem 1.1 (Qualitative complexity). For all coprime integers b2b\ge 2 and c2c\ge 2,

p(γb,c,b,n)n+(n).p(\gamma_{b,c},b,n)-n\longrightarrow +\infty \qquad (n\to\infty).

Theorem 1.2 (Quadratic lower bound). If α=logbc<2\alpha=\log_b c<2, then there exists n0=n0(b,c)n_0=n_0(b,c) such that

p(γb,c,b,n)(2α)216α2n2for all nn0.p(\gamma_{b,c},b,n)\ge \frac{(2-\alpha)^2}{16\alpha^2},n^2 \qquad\text{for all } n\ge n_0.

(We write α=logbc\alpha = \log_b c throughout the paper.) For a more striking application, we turn to the twisted Mahler constants. For integers d2d\ge 2, b2b\ge 2, c2c\ge 2 with gcd(b,c)=1\gcd(b,c)=1, define

Md,b,c  :=  k01ckbdk.M_{d,b,c} ;:=; \sum_{k\ge 0}\frac{1}{c^k,b^{,d^k}}.

These arise from the Mahler function h(x)=k0xdkh(x) = \sum_{k\ge 0} x^{d^k}, which satisfies h(x)=x+h(xd)h(x) = x + h(x^d); see Nishioka [Ni96] for background on Mahler functions in transcendence theory. When d3d\ge 3 and c>d2c > d^2, these constants lie beyond the reach of both prior approaches simultaneously. On the Diophantine side, μ(Md,b,c)=d\mu(M_{d,b,c}) = d (proved via the formal continued fraction of the associated Mahler function; see Badziahin [Bad19] and Rajchert [Raj24]), so μ3>2.510\mu \ge 3 > 2.510 and the Bugeaud--Kim threshold is exceeded. On the hot spot side, Bailey--Crandall [BC02] prove normality of Md,b,cM_{d,b,c} only when d>cd > \sqrt{c}; when c>d2c>d^2 this condition fails. Nevertheless:

Theorem 1.3 (μ\mu-bypass). For all d2d\ge 2, b2b\ge 2, c2c\ge 2 with gcd(b,c)=1\gcd(b,c)=1,

p(Md,b,c,b,n)n    +(n).p(M_{d,b,c},,b,,n)-n;\longrightarrow;+\infty \qquad(n\to\infty).

When d<cd < c, the exponential growth of the epoch lengths LK=(d1)dKL_K = (d-1)d^K allows a much stronger, quantitative conclusion:

Theorem 1.4 (Exponential lower bound). For all d2d\ge 2, b2b\ge 2, c2c\ge 2 with d<cd<c and gcd(b,c)=1\gcd(b,c)=1, there exists a constant C=C(d,b,c)C=C(d,b,c) such that

p(Md,b,c,b,n)    dn/αCp(M_{d,b,c},,b,,n) ;\ge; d^{,n/\alpha,-,C}

for all sufficiently large nn.

For comparison, the strongest quantitative result available from the Bugeaud--Kim method is lim supp(n)/n4/3\limsup, p(n)/n\ge 4/3 [BKK25], which applies only to constants satisfying a stringent irrationality exponent condition. Theorem 1.4 gives exponential growth in a regime where that method is provably inapplicable (see Remark 8.1).

All of the above are special cases of a general theorem. For integers b2b\ge 2, c2c\ge 2 with gcd(b,c)=1\gcd(b,c)=1, let f ⁣:NNf\colon\mathbb{N}\to\mathbb{N} be strictly increasing with LK:=f(K ⁣+ ⁣1)f(K)L_K:=f(K!+!1)-f(K)\to\infty, let g ⁣:NNg\colon\mathbb{N}\to\mathbb{N} be strictly increasing with g(K)g(K)\to\infty and g(K)=o(f(K))g(K)=o(f(K)), and let (ak)k1(a_k)_{k\ge 1} be integers with gcd(ak,c)=1\gcd(a_k,c)=1 for all kk. Assume further that

vc(bs1)<g(K)for all 1sLK and all large K.(1)v_c(b^s-1)<g(K) \qquad\text{for all }1\le s\le L_K\text{ and all large }K. \tag{1}

(A sufficient condition is logLK=o(g(K))\log L_K = o(g(K)), since vc(bs1)=O(logs)v_c(b^s-1)=O(\log s). When ff grows exponentially, (1) can instead be verified via multiplicative order estimates; see Corollary 7.2 and (8).) Define

ξ  =  k1akcg(k)bf(k).\xi;=;\sum_{k\ge 1}\frac{a_k}{c^{g(k)},b^{f(k)}}.

Theorem 1.5 (General epoch-expansion theorem). Under the hypotheses above, p(ξ,b,n)n+p(\xi,b,n)-n\to+\infty. Moreover, there exist constants C0=C0(b,c)C_0=C_0(b,c) and K0=K0(b,c,f,g)K_0=K_0(b,c,f,g) such that for all sufficiently large nn,

p(ξ,b,n)    K=AnBn(LKn+1),p(\xi,b,n);\ge;\sum_{K=A_n}^{B_n}(L_K - n + 1),

where An=min{KK0:LKn}A_n=\min{K\ge K_0: L_K\ge n} and Bn=max{K:g(K)α+C0<n}B_n=\max{K: g(K)\alpha + C_0 < n}. When Bn<AnB_n < A_n (which can happen for slowly growing ff with α2\alpha \ge 2), the qualitative conclusion p(ξ,b,n)n+p(\xi,b,n)-n\to+\infty still holds via the Cassaigne argument of Theorem 1.1, applied with g(K)g(K) in place of KK.

The quantitative bound mirrors the spacing function: quadratic spacing (f(k)=k2f(k)=k^2) gives p(n)c0n2p(n)\ge c_0 n^2; exponential spacing (f(k)=dkf(k)=d^k) gives p(n)dn/αCp(n)\ge d^{n/\alpha-C}. Theorems 1.1, 1.2, and 1.4 are corollaries of Theorem 1.5 (see Section 7); Theorem 1.3 requires an independent argument given in Section 8.

Proof architecture

We present the proofs for the partial theta values γb,c\gamma_{b,c} independently of the general theorem, because they introduce the key ideas in a concrete setting. The architecture of the general proof is as follows.

All results rest on the epoch-expansion framework, whose applicability is determined by the structural properties of ξ=ak/(cg(k)bf(k))\xi=\sum a_k/(c^{g(k)}b^{f(k)}): coprime denominator (gcd(b,c)=1\gcd(b,c)=1, giving a cc-adic lattice structure for the orbit); increasing gaps (LKL_K \to \infty, creating epochs of growing length); single-modulus lattice (all terms share the modulus cc, making vc(bs1)v_c(b^s-1) the sole obstruction to digit agreement); and valuation control (condition (1)).

Given these properties, the proof operates in two modes. For the qualitative conclusion (p(n)np(n)-n\to\infty), we argue by contradiction: if p(n)np(n)-n were bounded, Cassaigne's theorem [Ca97] would force the digit sequence to be quasi-Sturmian, producing long self-matches at certain gaps. We place such a matched pair inside a single large epoch and show that the within-epoch valuation bound limits the match length to O(Kα)O(K\alpha), contradicting the Sturmian match length qk+1\gg q_{k+1} since K=O(logqk+1)K=O(\log q_{k+1}). For the quantitative conclusion, we count distinct length-nn subwords directly: each epoch of length LKnL_K \ge n contributes LK\sim L_K starting positions whose length-nn subwords are pairwise distinct (by the valuation bound within epochs, and by the lattice gap across epochs), and summing over eligible epochs yields the lower bound.

Further applications

Beyond partial theta values and twisted Mahler constants, Theorem 1.5 applies uniformly to every lacunary constant satisfying the hypotheses above:

(a) Tschakaloff function values Tb(1/c)=k11/(ckbk(k+1)/2)T_b(1/c)=\sum_{k\ge 1}1/(c^k b^{k(k+1)/2}) (f(k)=k(k+1)/2f(k)=k(k+1)/2, LK=K+1L_K=K+1; quadratic bound).

(b) Fibonacci-exponent constants k11/(ckbFk)\sum_{k\ge 1}1/(c^k b^{F_k}) (f(k)=Fkf(k)=F_k, LK=FK1L_K=F_{K-1}; exponential bound p(n)φn/αCp(n)\ge \varphi^{n/\alpha-C} when α\alpha is sufficiently small).

(c) Signed coefficients ak{±1}a_k\in{\pm 1} (gcd(±1,c)=1\gcd(\pm 1,c)=1 always); this covers values of Rogers false theta functions at rational arguments.

Organization

Section 2 collects notation and the Sturmian input. Section 3 gives the epoch decomposition of the orbit {bnγb,c}{b^n\gamma_{b,c}}. Section 4 proves the within-epoch and cross-epoch match bounds. Theorems 1.1 and 1.2 are proved in Sections 5 and 6. Section 7 states and proves the general epoch-expansion theorem (Theorem 1.5) and derives applications to Tschakaloff function values, Fibonacci-exponent constants, and signed-coefficient series. Section 8 treats twisted Mahler constants, proving Theorems 1.3 and 1.4; this includes the exponential bound in the μ\mu-bypass regime d3d\ge 3, c>d2c>d^2 where both prior methods are provably inapplicable. Section 9 discusses open questions.


2. Preliminaries

Throughout the paper, b2b\ge 2 and c2c\ge 2 are fixed coprime integers, and

α=logbc>0.\alpha=\log_b c>0.

2.1. Digits, orbit points, and complexity

For xRx\in\mathbb{R}, we write x\lfloor x \rfloor for the floor and {x}=xx{x}=x-\lfloor x \rfloor for the fractional part.

We consider

γb,c=k11ckbk2,\gamma_{b,c}=\sum_{k\ge 1}\frac{1}{c^k b^{k^2}},

and its orbit under multiplication by bb:

zn:={bnγb,c},n0.z_n:={b^n\gamma_{b,c}},\qquad n\ge 0.

The base-bb digit sequence of γb,c\gamma_{b,c} is then

xn=bzn1,n1,x_n=\lfloor b z_{n-1} \rfloor,\qquad n\ge 1,

so that

γb,c=n1xnbn.\gamma_{b,c}=\sum_{n\ge 1} x_n b^{-n}.

Definition 2.1. For n1n\ge 1, the subword complexity of γb,c\gamma_{b,c} in base bb is

p(γb,c,b,n)=#{xi+1xi+2xi+n:i0}.p(\gamma_{b,c},b,n) = #\bigl{x_{i+1}x_{i+2}\cdots x_{i+n}: i\ge 0\bigr}.

When the parameters are clear, we abbreviate this to p(n)p(n).

2.2. Match length

Definition 2.2. Let w=(wn)n1\mathbf{w}=(w_n)_{n\ge 1} be an infinite word over a finite alphabet. For n1n\ge 1 and g1g\ge 1, the match length at position nn with gap gg is

Matchw(n,g)=max{L0:wn+j=wn+g+j for all 0j<L}.\operatorname{Match}{\mathbf{w}}(n,g) = \max\bigl{L\ge 0 : w{n+j}=w_{n+g+j}\ \text{for all }0\le j<L\bigr}.

For the digit sequence x=(xn)n1\mathbf{x}=(x_n){n\ge 1} of γb,c\gamma{b,c}, we write

M(n,g):=Matchx(n+1,g),n0, g1.M(n,g):=\operatorname{Match}_{\mathbf{x}}(n+1,g), \qquad n\ge 0,\ g\ge 1.

Equivalently, M(n,g)M(n,g) is the largest L0L\ge 0 such that the first LL base-bb digits of znz_n and zn+gz_{n+g} coincide.

2.3. Square epochs

For K1K\ge 1, define epoch KK to be the interval of positions

[K2,(K+1)2).[K^2,(K+1)^2).

Its length is

LK=(K+1)2K2=2K+1.L_K=(K+1)^2-K^2=2K+1.

If nn lies in epoch KK, we write

en:=(K+1)2n,1en2K+1,e_n:=(K+1)^2-n, \qquad 1\le e_n\le 2K+1,

for the distance from nn to the next epoch boundary.

2.4. cc-adic valuation

Let

c=p1a1prarc=p_1^{a_1}\cdots p_r^{a_r}

be the prime factorization of cc. For a nonzero integer mm, define

vc(m):=min1irvpi(m)ai,v_c(m):= \min_{1\le i\le r}\left\lfloor\frac{v_{p_i}(m)}{a_i}\right\rfloor,

so that vc(m)v_c(m) is the largest k0k\ge 0 such that ckmc^k\mid m. We set vc(0)=+v_c(0)=+\infty.

2.5. Cassaigne's theorem

A Sturmian word is an aperiodic binary word of minimal complexity, namely p(n)=n+1p(n)=n+1 for all n1n\ge 1. A word is quasi-Sturmian if its complexity is bounded above by n+Cn+C for some constant CC.

We use the following theorem of Cassaigne.

Theorem 2.3 (Cassaigne [Ca97]). For a non-eventually-periodic infinite word u\mathbf{u} over a finite alphabet, the following are equivalent:

(i) lim infn(pu(n)n)<\liminf_{n\to\infty}(p_{\mathbf{u}}(n)-n)<\infty;

(ii) u\mathbf{u} is eventually quasi-Sturmian, i.e. there exist a finite word WW, a Sturmian word s\mathbf{s} over {0,1}{0,1}, and a morphism

φ:{0,1}A\varphi:{0,1}\to \mathcal{A}^*

such that

u=Wφ(s).\mathbf{u}=W,\varphi(\mathbf{s}).

2.6. Two Sturmian lemmas

The first lemma is the source of long local self-matches in a Sturmian word. Here Matchs(n,g)\operatorname{Match}_{\mathbf{s}}(n,g) denotes the match length of Section 2 applied to the Sturmian word s\mathbf{s}.

Lemma 2.4 (Strong Sturmian match). Let s\mathbf{s} be a Sturmian word of slope β\beta, and let qkq_k be the denominators of the convergents of β\beta. For all sufficiently large kk, there exists

nk[qk+1/2, qk+1)n_k\in [q_{k+1}/2,\ q_{k+1})

such that

Matchs(nk+1,qk)qk+1/16.\operatorname{Match}{\mathbf{s}}(n_k+1,q_k)\ge \lfloor q{k+1}/16\rfloor.

Proof. Let εk=qkβ\varepsilon_k=|q_k\beta|. By continued-fraction theory,

1qk+1+qk<εk<1qk+1,\frac{1}{q_{k+1}+q_k}<\varepsilon_k<\frac{1}{q_{k+1}},

hence εk>1/(2qk+1)\varepsilon_k>1/(2q_{k+1}) for large kk.

A mismatch at shift qkq_k among the first mm symbols can occur only if the starting point of the coding orbit falls within distance εk\varepsilon_k of one of the mm discontinuity preimages. Thus the set of bad starting points is covered by at most mm intervals of total length at most 2mεk2m\varepsilon_k.

Among the qk+1q_{k+1} points {jβ}{j\beta}, 0j<qk+10\le j<q_{k+1}, the minimum spacing is at least εk>1/(2qk+1)\varepsilon_k>1/(2q_{k+1}). Therefore the number of bad starting points among these qk+1q_{k+1} orbit points is at most

2mεk2qk+1+m5m.2m\varepsilon_k\cdot 2q_{k+1}+m\le 5m.

Take m=qk+1/16m=\lfloor q_{k+1}/16 \rfloor. Then at least

qk+15m1116qk+1q_{k+1}-5m\ge \frac{11}{16}q_{k+1}

starting points have match length at least mm. In particular, one such point lies in [qk+1/2, qk+1)[q_{k+1}/2,\ q_{k+1}). ∎

The second lemma is a standard recurrence property of Sturmian words.

Lemma 2.5 (Recurrence of Sturmian factors). Let s\mathbf{s} be a Sturmian word with convergent denominators qkq_k. For [qk,qk+1)\ell \in [q_k, q_{k+1}), the recurrence function satisfies

R()    qk+1+qk1.R(\ell) ;\le; q_{k+1} + q_k - 1.

In particular, every factor of length \ell occurs in every block of length qk+1+qkq_{k+1} + q_k.

Proof. See [Lo02, Ch. 2, Prop. 2.2.22]. ∎


3. Epoch decomposition and irrationality

We begin with the basic decomposition of znz_n inside a square epoch.

Lemma 3.1 (Epoch decomposition). Let nn lie in epoch KK, so that K2n<(K+1)2K^2\le n<(K+1)^2. Then

zn=PncK+Tn,(2)z_n=\frac{P_n}{c^K}+T_n, \tag{2}

where:

(a) PnP_n is an integer with 0Pn<cK0\le P_n<c^K and

PnbnK2(modc),P_n\equiv b^{,n-K^2}\pmod c,

hence gcd(Pn,c)=1\gcd(P_n,c)=1;

(b)

Tn=t11cK+tbun,t,un,t:=(K+t)2n=en+(t1)(2K+t+1).T_n=\sum_{t\ge 1}\frac{1}{c^{K+t} b^{u_{n,t}}}, \qquad u_{n,t}:=(K+t)^2-n =e_n+(t-1)(2K+t+1).

In particular,

0<Tn16151cK+1ben,(3)0<T_n\le \frac{16}{15},\frac{1}{c^{K+1}b^{e_n}}, \tag{3}

and

0<Tn1cK+1ben16151cK+2ben+2K+3.(4)0<T_n-\frac{1}{c^{K+1}b^{e_n}} \le \frac{16}{15},\frac{1}{c^{K+2}b^{e_n+2K+3}}. \tag{4}

Proof. Write

bnγb,c=j=1Kbnj2cj+j>Kbnj2cj.b^n\gamma_{b,c} = \sum_{j=1}^{K}\frac{b^{n-j^2}}{c^j} + \sum_{j>K}\frac{b^{n-j^2}}{c^j}.

Set

Qn:=j=1KcKjbnj2Z.Q_n:=\sum_{j=1}^{K} c^{K-j} b^{n-j^2}\in \mathbb{Z}.

Then

bnγb,c=QncK+Tn,Tn:=j>Kbnj2cj.b^n\gamma_{b,c}=\frac{Q_n}{c^K}+T_n, \qquad T_n:=\sum_{j>K}\frac{b^{n-j^2}}{c^j}.

Let PnP_n be the residue of QnQ_n modulo cKc^K in [0,cK)[0,c^K). By (3) below and en1e_n \ge 1, 0<Tn<1/cK0 < T_n < 1/c^K. Since 0Pn<cK0 \le P_n < c^K, we have Pn/cK+Tn<(cK1)/cK+1/cK=1P_n/c^K + T_n < (c^K - 1)/c^K + 1/c^K = 1. Taking fractional parts therefore yields

zn=PncK+Tn.z_n=\frac{P_n}{c^K}+T_n.

Modulo cc, every term in QnQ_n with j<Kj<K vanishes, while the term j=Kj=K equals bnK2b^{n-K^2}. Thus

PnQnbnK2(modc),P_n\equiv Q_n\equiv b^{n-K^2}\pmod c,

and since gcd(b,c)=1\gcd(b,c)=1, we also have gcd(Pn,c)=1\gcd(P_n,c)=1.

For the tail, write j=K+tj=K+t with t1t\ge 1. Then

Tn=t11cK+tb(K+t)2n=t11cK+tbun,t.T_n = \sum_{t\ge 1}\frac{1}{c^{K+t} b^{(K+t)^2-n}} = \sum_{t\ge 1}\frac{1}{c^{K+t} b^{u_{n,t}}}.

Since

un,t=en+(t1)(2K+t+1)en+(t1)(2K+3),u_{n,t}=e_n+(t-1)(2K+t+1)\ge e_n+(t-1)(2K+3),

we get

Tn1cK+1bent0(1cb2K+3)t.T_n \le \frac{1}{c^{K+1}b^{e_n}} \sum_{t\ge 0}\left(\frac{1}{cb^{2K+3}}\right)^t.

As cb2K+316cb^{2K+3}\ge 16, the geometric series is bounded by 16/1516/15, which proves (3).

The same argument starting from t=2t=2 gives

Tn1cK+1ben1cK+2ben+2K+3u0(1cb2K+5)u16151cK+2ben+2K+3.T_n-\frac{1}{c^{K+1}b^{e_n}} \le \frac{1}{c^{K+2}b^{e_n+2K+3}} \sum_{u\ge 0}\left(\frac{1}{cb^{2K+5}}\right)^u \le \frac{16}{15},\frac{1}{c^{K+2}b^{e_n+2K+3}}.

This proves (4). ∎

Lemma 3.2. The number γb,c\gamma_{b,c} is irrational.

Proof. Let

SK:=k=1K1ckbk2.S_K:=\sum_{k=1}^{K}\frac{1}{c^k b^{k^2}}.

Its denominator divides

DK:=cKbK2.D_K:=c^K b^{K^2}.

Moreover,

0<γb,cSKjK+11cjbj22cK+1b(K+1)2=2DK+10<\gamma_{b,c}-S_K \le \sum_{j\ge K+1}\frac{1}{c^j b^{j^2}} \le \frac{2}{c^{K+1}b^{(K+1)^2}} = \frac{2}{D_{K+1}}

for KK large.

If γb,c=p/qQ\gamma_{b,c}=p/q\in\mathbb{Q} and SKp/qS_K\ne p/q, then

1qDKγb,cSK2DK+1.\frac{1}{qD_K}\le \left|\gamma_{b,c}-S_K\right|\le \frac{2}{D_{K+1}}.

Hence DK+12qDKD_{K+1}\le 2qD_K, which is impossible for large KK because

DK+1DK=cb2K+1.\frac{D_{K+1}}{D_K}=c,b^{2K+1}\to\infty.

If instead SK=p/qS_K=p/q for all large KK, then SK+1>SKS_{K+1}>S_K, again impossible. ∎


4. Match bounds

4.1. A basic comparison principle

If two numbers in [0,1)[0,1) have the same first LL base-bb digits, then they belong to the same bb-adic interval of length bLb^{-L}. Therefore, whenever znzn+sz_n\ne z_{n+s},

M(n,s)logb ⁣(1/znzn+s).(5)M(n,s)\le \log_b!\bigl(1/|z_n-z_{n+s}|\bigr). \tag{5}

4.2. Within one epoch

Theorem 4.1 (Within-epoch match bound). There exist constants Kwe=Kwe(b,c)K_{\mathrm{we}}=K_{\mathrm{we}}(b,c) and Cwe=Cwe(b,c)C_{\mathrm{we}}=C_{\mathrm{we}}(b,c) such that the following holds.

Let KKweK\ge K_{\mathrm{we}}, and let n,n+sn,n+s lie in the same epoch KK with 1s2K+11\le s\le 2K+1. Then

M(n,s)Kα+Cwe.M(n,s)\le K\alpha + C_{\mathrm{we}}.

Proof. Let e=en=(K+1)2ne=e_n=(K+1)^2-n. Since n+sn+s also lies in epoch KK, we have

en+s=es1,hencees+1.e_{n+s}=e-s\ge 1, \qquad\text{hence}\qquad e\ge s+1.

By Lemma 3.1,

zn=PncK+Tn,zn+s=Pn+scK+Tn+s,z_n=\frac{P_n}{c^K}+T_n, \qquad z_{n+s}=\frac{P_{n+s}}{c^K}+T_{n+s},

with 0Pn,Pn+s<cK0\le P_n,P_{n+s}<c^K. Set

Δ:=PnPn+s.\Delta:=P_n-P_{n+s}.

Then

znzn+s=ΔcK+(TnTn+s).(6)z_n-z_{n+s}=\frac{\Delta}{c^K}+(T_n-T_{n+s}). \tag{6}

To understand Δ\Delta, define

Qm:=j=1KcKjbmj2Z(m=n,n+s).Q_m:=\sum_{j=1}^{K} c^{K-j} b^{m-j^2}\in \mathbb{Z} \qquad (m=n,n+s).

Then QmPm(modcK)Q_m\equiv P_m\pmod{c^K}, and

Qn+s=bsQn.Q_{n+s}=b^sQ_n.

Hence

Pn+sbsPn(modcK),P_{n+s}\equiv b^s P_n\pmod{c^K},

so

Δ(1bs)Pn(modcK).(7)\Delta\equiv (1-b^s)P_n\pmod{c^K}. \tag{7}

Set

ν:=vc(bs1).\nu:=v_c(b^s-1).

Since 1s2K+11\le s\le 2K+1, one has ν=O(logK)\nu=O(\log K). Indeed, if pcp\mid c is a fixed prime factor of cc and d0=ordp(b)d_0=\operatorname{ord}_p(b), then the standard pp-adic valuation formula vp(bs1)=vp(bd01)+vp(s/d0)v_p(b^s-1)=v_p(b^{d_0}-1)+v_p(s/d_0) (when d0sd_0\mid s; zero otherwise) gives

vp(bs1)Ap+logpsv_p(b^s-1)\le A_p+\log_p s

for a constant Ap=Ap(b)A_p=A_p(b). As cν(bs1)c^\nu\mid (b^s-1) implies pν(bs1)p^\nu\mid (b^s-1), we get

νvp(bs1)Ap+logp(2K+1)=O(logK).\nu\le v_p(b^s-1)\le A_p+\log_p(2K+1)=O(\log K).

Thus ν<K\nu<K for all KKweK\ge K_{\mathrm{we}}.

Now (7) and gcd(Pn,c)=1\gcd(P_n,c)=1 imply

vc(Δ)=vc(bs1)=ν,v_c(\Delta)=v_c(b^s-1)=\nu,

because divisibility by crc^r with r<Kr<K is preserved under congruence modulo cKc^K. In particular, Δ0\Delta\ne 0, and therefore

ΔcK1cKν.()\left|\frac{\Delta}{c^K}\right|\ge \frac{1}{c^{K-\nu}}. \tag{}

Next, since nn and n+sn+s lie in the same epoch,

Tn+s=bsTn.T_{n+s}=b^s T_n.

Using Lemma 3.1 and es+1e\ge s+1,

TnTn+s=(bs1)Tn1615bs1cK+1be16151cK+1b.|T_n-T_{n+s}|=(b^s-1)T_n \le \frac{16}{15},\frac{b^s-1}{c^{K+1}b^e} \le \frac{16}{15},\frac{1}{c^{K+1}b}.

Combining this with (6) and (*),

znzn+s1cKν16151cK+1b=1cKν(11615cν+1b).|z_n-z_{n+s}| \ge \frac{1}{c^{K-\nu}}-\frac{16}{15},\frac{1}{c^{K+1}b} = \frac{1}{c^{K-\nu}} \left(1-\frac{16}{15c^{\nu+1}b}\right).

Since b,c2b,c\ge 2,

1615cν+1b161522=415<12.\frac{16}{15c^{\nu+1}b}\le \frac{16}{15\cdot 2\cdot 2}=\frac{4}{15}<\frac12.

Therefore

znzn+s12cKν.|z_n-z_{n+s}|\ge \frac{1}{2c^{K-\nu}}.

By (5),

M(n,s)logb(2cKν)Kα+logb2.M(n,s)\le \log_b(2c^{K-\nu})\le K\alpha+\log_b 2.

This proves the theorem. ∎

4.3. A local cross-epoch bound

The next proposition is the local estimate needed in the qualitative proof. The hypothesis on the epoch gap δ\delta is the only place where the quantity

D(K1):=min ⁣(K1+2, 2K1+2α)D(K_1):=\min!\left(K_1+2,\ \left\lfloor\frac{2K_1+2}{\alpha}\right\rfloor\right)

appears.

Proposition 4.2 (Local cross-epoch bound). There exist constants Kloc=Kloc(b,c)K_{\mathrm{loc}}=K_{\mathrm{loc}}(b,c) and Cloc=Cloc(b,c)C_{\mathrm{loc}}=C_{\mathrm{loc}}(b,c) such that the following holds.

Let NN lie in epoch K1K_1, let N+sN+s lie in a later epoch K2>K1K_2>K_1, and set

δ:=K2K1,e1:=(K1+1)2N,e2:=(K2+1)2(N+s).\delta:=K_2-K_1,\qquad e_1:=(K_1+1)^2-N,\qquad e_2:=(K_2+1)^2-(N+s).

Assume

1s3NandδD(K1).1\le s\le 3N \qquad\text{and}\qquad \delta\le D(K_1).

Then for all K1KlocK_1\ge K_{\mathrm{loc}},

M(N,s)(K2+1)α+max(e1,e2)+Cloc.M(N,s)\le (K_2+1)\alpha + \max(e_1,e_2)+C_{\mathrm{loc}}.

In particular,

M(N,s)=O(N).M(N,s)=O(\sqrt N).

Proof. By Lemma 3.1,

zN=P1cK1+T1,zN+s=P2cK2+T2,z_N=\frac{P_1}{c^{K_1}}+T_1, \qquad z_{N+s}=\frac{P_2}{c^{K_2}}+T_2,

where gcd(P1,c)=gcd(P2,c)=1\gcd(P_1,c)=\gcd(P_2,c)=1. Set

D:=cδP1P2.D:=c^\delta P_1-P_2.

Then cDc\nmid D (because ccδP1c\mid c^\delta P_1 but cP2c\nmid P_2), hence D0D\ne 0, and

zNzN+s=DcK2+T1T2.z_N-z_{N+s}=\frac{D}{c^{K_2}}+T_1-T_2.

Extract the first tail term at each position:

T1=1cK1+1be1+R1,T2=1cK2+1be2+R2.T_1=\frac{1}{c^{K_1+1}b^{e_1}}+R_1, \qquad T_2=\frac{1}{c^{K_2+1}b^{e_2}}+R_2.

By (4),

R116151cK1+2be1+2K1+3,R216151cK2+2be2+2K2+3.()|R_1| \le \frac{16}{15},\frac{1}{c^{K_1+2}b^{e_1+2K_1+3}}, \qquad |R_2| \le \frac{16}{15},\frac{1}{c^{K_2+2}b^{e_2+2K_2+3}}. \tag{}

Thus

zNzN+s=DcK2+1cK1+1be11cK2+1be2+(R1R2).z_N-z_{N+s} = \frac{D}{c^{K_2}} +\frac{1}{c^{K_1+1}b^{e_1}} -\frac{1}{c^{K_2+1}b^{e_2}} +(R_1-R_2).

We split into three cases.

Case 1: e1e2e_1\ge e_2. Multiply by cK1+1be1c^{K_1+1}b^{e_1}:

cK1+1be1(zNzN+s)=cDbe1+cδbe1e2cδ+E.c^{K_1+1}b^{e_1}(z_N-z_{N+s}) = \frac{cDb^{e_1}+c^\delta-b^{e_1-e_2}}{c^\delta}+E.

Here E:=cK1+1be1(R1R2)E:=c^{K_1+1}b^{e_1}(R_1-R_2). The numerator of the rational part is congruent modulo cc to be1e2-b^{e_1-e_2}, hence is not divisible by cc. Therefore the rational part is at distance at least cδc^{-\delta} from Z\mathbb{Z}.

We now estimate the error. From (**),

E16151cb2K1+3+16151cδ+1be2+2K2+3e1.|E| \le \frac{16}{15},\frac{1}{cb^{2K_1+3}} +\frac{16}{15},\frac{1}{c^{\delta+1}b^{e_2+2K_2+3-e_1}}.

Since e12K1+1e_1\le 2K_1+1 and e21e_2\ge 1,

e2+2K2+3e11+2(K1+δ)+3(2K1+1)=2δ+35,e_2+2K_2+3-e_1\ge 1+2(K_1+\delta)+3-(2K_1+1)=2\delta+3\ge 5,

so the second term is at most (16/15)c(δ+1)b5(16/15)c^{-(\delta+1)}b^{-5}.

For the first term, the hypothesis δD(K1)\delta\le D(K_1) gives αδ2K1+2\alpha \delta\le 2K_1+2, hence cδ=bαδb2K1+2c^\delta=b^{\alpha \delta}\le b^{2K_1+2}. Therefore

16151cb2K1+316151cbcδ=1615cbcδ415cδ.\frac{16}{15},\frac{1}{cb^{2K_1+3}} \le \frac{16}{15},\frac{1}{cb,c^\delta} = \frac{16}{15cb},c^{-\delta} \le \frac{4}{15},c^{-\delta}.

Also

16151cδ+1b5115cδ.\frac{16}{15},\frac{1}{c^{\delta+1}b^5} \le \frac{1}{15},c^{-\delta}.

Thus E13cδ|E|\le \frac13 c^{-\delta}, and hence

zNzN+s231cK2+1be1.|z_N-z_{N+s}| \ge \frac{2}{3},\frac{1}{c^{K_2+1}b^{e_1}}.

Case 2: e1<e2e_1<e_2 and δ2\delta\ge 2. Again multiply by cK1+1be1c^{K_1+1}b^{e_1}:

cK1+1be1(zNzN+s)=Dbe1cδ1+1+E,c^{K_1+1}b^{e_1}(z_N-z_{N+s}) = \frac{Db^{e_1}}{c^{\delta-1}}+1+E,

where

E=1cδbe2e1+cK1+1be1(R1R2).E= -\frac{1}{c^\delta b^{e_2-e_1}} + c^{K_1+1}b^{e_1}(R_1-R_2).

Because cDc\nmid D and gcd(b,c)=1\gcd(b,c)=1, the rational term Dbe1/cδ1Db^{e_1}/c^{\delta-1} has exact denominator cδ1c^{\delta-1}, so

dist ⁣(Dbe1cδ1+1, Z)c(δ1).\operatorname{dist}!\left(\frac{Db^{e_1}}{c^{\delta-1}}+1,\ \mathbb{Z}\right)\ge c^{-(\delta-1)}.

Using (**) and e2e11e_2-e_1\ge 1,

E1cδb+16151cb2K1+3+16151cδ+1be2+2K2+3e1.|E| \le \frac{1}{c^\delta b} +\frac{16}{15},\frac{1}{cb^{2K_1+3}} +\frac{16}{15},\frac{1}{c^{\delta+1}b^{e_2+2K_2+3-e_1}}.

As above, cδb2K1+2c^\delta\le b^{2K_1+2}, so

16151cb2K1+316151c2bc(δ1)215c(δ1).\frac{16}{15},\frac{1}{cb^{2K_1+3}} \le \frac{16}{15},\frac{1}{c^2 b},c^{-(\delta-1)} \le \frac{2}{15},c^{-(\delta-1)}.

Also

1cδb1cbc(δ1)14c(δ1).\frac{1}{c^\delta b}\le \frac{1}{cb},c^{-(\delta-1)}\le \frac14,c^{-(\delta-1)}.

Finally, since e2+2K2+3e12δ+48e_2+2K_2+3-e_1\ge 2\delta+4\ge 8,

16151cδ+1be2+2K2+3e1115c(δ1).\frac{16}{15},\frac{1}{c^{\delta+1}b^{e_2+2K_2+3-e_1}} \le \frac{1}{15},c^{-(\delta-1)}.

Hence E<12c(δ1)|E|<\frac12 c^{-(\delta-1)}, and therefore

zNzN+s12cK2be1.|z_N-z_{N+s}| \ge \frac{1}{2c^{K_2}b^{e_1}}.

Case 3: δ=1\delta=1 and e1<e2e_1<e_2. Multiply by cK1+1be2c^{K_1+1}b^{e_2}:

cK1+1be2(zNzN+s)=Dbe2+be2e11c+E,c^{K_1+1}b^{e_2}(z_N-z_{N+s}) = Db^{e_2}+b^{e_2-e_1}-\frac{1}{c}+E,

where E:=cK1+1be2(R1R2)E:=c^{K_1+1}b^{e_2}(R_1-R_2). The displayed integer part is at distance exactly 1/c1/c from Z\mathbb{Z}.

Since δ=1\delta=1, we have

s=(K2+1)2(K1+1)2+e1e2=2K1+3+e1e21,s=(K_2+1)^2-(K_1+1)^2+e_1-e_2=2K_1+3+e_1-e_2\ge 1,

so e2e12K1+2e_2-e_1\le 2K_1+2. Hence, by (**),

E16151cb2K1+3(e2e1)+16151c2b2K2+316151cb+160c<35c.|E| \le \frac{16}{15},\frac{1}{cb^{,2K_1+3-(e_2-e_1)}} +\frac{16}{15},\frac{1}{c^2 b^{2K_2+3}} \le \frac{16}{15},\frac{1}{cb} +\frac{1}{60c} < \frac{3}{5c}.

Therefore

zNzN+s251cK2+1be2.|z_N-z_{N+s}| \ge \frac{2}{5},\frac{1}{c^{K_2+1}b^{e_2}}.

In all three cases we have

zNzN+s1C1cK2+1bmax(e1,e2)|z_N-z_{N+s}| \ge \frac{1}{C},\frac{1}{c^{K_2+1}b^{\max(e_1,e_2)}}

for an absolute constant C=C(b,c)C=C(b,c). By (5),

M(N,s)(K2+1)α+max(e1,e2)+logbC.M(N,s)\le (K_2+1)\alpha+\max(e_1,e_2)+\log_b C.

This proves the proposition. ∎

Remark 4.3. If α<2\alpha<2, then D(K1)=K1+2D(K_1)=K_1+2 for all large K1K_1, so the hypothesis δD(K1)\delta\le D(K_1) is automatic from s3Ns\le 3N. For general α\alpha, the qualitative proof below uses the recurrence of Sturmian factors to place the repeated pattern so that δD(K1)\delta\le D(K_1) still holds. The restriction α<2\alpha<2 is needed only for the quantitative Theorem 1.2.


5. Proof of Theorem 1.1

Proof. Assume for contradiction that

lim infn(p(γb,c,b,n)n)<.\liminf_{n\to\infty}\bigl(p(\gamma_{b,c},b,n)-n\bigr)<\infty.

By Lemma 3.2, the number γb,c\gamma_{b,c} is irrational. Hence its digit sequence is not eventually periodic, and by Theorem 2.3 it is eventually quasi-Sturmian:

x=Wφ(s),\mathbf{x}=W,\varphi(\mathbf{s}),

where WW is a finite word, s\mathbf{s} is a Sturmian word of slope β\beta, and

φ:{0,1}{0,1,,b1}\varphi:{0,1}\to {0,1,\dots,b-1}^*

is a morphism. Since γb,c\gamma_{b,c} is irrational, φ\varphi must be non-erasing: if φ(i)=0|\varphi(i)|=0 for some i{0,1}i\in{0,1}, then pφ(s)(n)φ(1i)p_{\varphi(\mathbf{s})}(n)\le |\varphi(1-i)| for all nφ(1i)n\ge|\varphi(1-i)|, contradicting p(n)n+1p(n)\ge n+1 from irrationality.

Write

l0:=φ(0),l1:=φ(1),lmin:=min(l0,l1)1,l_0:=|\varphi(0)|,\qquad l_1:=|\varphi(1)|,\qquad l_{\min}:=\min(l_0,l_1)\ge 1,

and let

λ:=(1β)l0+βl1.\lambda:=(1-\beta)l_0+\beta l_1.

If F(m)F(m) denotes the number of digits in the prefix Wφ(s1sm)W\varphi(s_1\cdots s_m), then the Sturmian balance property implies

F(m)=λm+O(1).F(m)=\lambda m+O(1).

Consequently, there exists a constant B1B\ge 1 such that for all m,q0m,q\ge 0,

F(m)λmB,F(m+q)F(m)λq2B.(9)|F(m)-\lambda m|\le B, \qquad |F(m+q)-F(m)-\lambda q|\le 2B. \tag{9}

Let β=[0;a1,a2,]\beta = [0; a_1, a_2, \ldots] be the continued-fraction expansion of the Sturmian slope, and let qkq_k denote the convergent denominators. We distinguish two cases according to whether the partial quotients aka_k are bounded.

Case A: supkak=\sup_k a_k = \infty. There exist infinitely many kk with ak+12αa_{k+1} \ge \lceil 2\alpha \rceil. For such kk,

qkqk+1    1ak+1    12α.\frac{q_k}{q_{k+1}} ;\le; \frac{1}{a_{k+1}} ;\le; \frac{1}{2\alpha}.

Lemma 2.4 gives nk[qk+1/2,  qk+1)n_k \in [q_{k+1}/2,; q_{k+1}) with Matchs(nk ⁣+ ⁣1,qk)qk+1/16\operatorname{Match}{\mathbf{s}}(n_k!+!1, q_k) \ge q{k+1}/16.

Set Nk:=F(nk)N_k := F(n_k) and Gk:=F(nk+qk)F(nk)G_k := F(n_k + q_k) - F(n_k). By (9),

Nk    λqk+1+B,Gk    λqk+2B.N_k ;\le; \lambda q_{k+1} + B, \qquad G_k ;\le; \lambda q_k + 2B.

Since nkqk+1/2n_k \ge q_{k+1}/2, also Nkλqk+1/2BN_k \ge \lambda q_{k+1}/2 - B. Hence for large kk,

GkNk    λqk+2Bλqk+1/2B    (2+ε)qkqk+1    2+ε2α\frac{G_k}{N_k} ;\le; \frac{\lambda q_k + 2B}{\lambda q_{k+1}/2 - B} ;\le; (2+\varepsilon),\frac{q_k}{q_{k+1}} ;\le; \frac{2+\varepsilon}{2\alpha}

for any ε>0\varepsilon>0 and all sufficiently large kk. When α2\alpha\ge 2, this gives Gk/Nk(1+ε)/αG_k/N_k\le (1+\varepsilon)/\alpha for small ε>0\varepsilon>0, which suffices for the epoch-gap bound below. When α<2\alpha<2, the ratio Gk/Nk<1/αG_k/N_k<1/\alpha is not needed: since Gkλqk+2Bλqk+1+2B2(λqk+1/2+B)2(Nk+2B)3NkG_k\le \lambda q_k+2B\le \lambda q_{k+1}+2B\le 2(\lambda q_{k+1}/2+B)\le 2(N_k+2B)\le 3N_k for kk sufficiently large, and Nk+Gk4Nk<4(K1,k+1)2N_k+G_k\le 4N_k<4(K_{1,k}+1)^2, we get dkK1,k+2=D(K1,k)d_k\le K_{1,k}+2=D(K_{1,k}) directly.

The morphic transfer gives a digit match of length Lklminqk+1/16L_k \ge l_{\min} \lfloor q_{k+1}/16 \rfloor. Using the upper bound Nk2λqk+1N_k \le 2\lambda q_{k+1} (for large kk): Lklminqk+1/32c1NkL_k \ge l_{\min} q_{k+1}/32 \ge c_1 N_k where c1:=lmin/(64λ)>0c_1 := l_{\min}/(64\lambda) > 0.

Case B: supkak=M<\sup_k a_k = M < \infty. All partial quotients satisfy akMa_k \le M. Then the Sturmian word s\mathbf{s} is linearly recurrent: for every factor of length \ell, R()(M ⁣+ ⁣2)R(\ell) \le (M!+!2),\ell (since R()qj+1+qjR(\ell) \le q_{j+1} + q_j for [qj,qj+1)\ell \in [q_j, q_{j+1}), and qj+1/qjaj+1 ⁣+ ⁣1M ⁣+ ⁣1q_{j+1}/q_j \le a_{j+1}!+!1 \le M!+!1).

Fix

A:=2α(M ⁣+ ⁣2)+M+2.A := 2\alpha(M!+!2) + M + 2.

By Lemma 2.4, for large kk there exists nk[qk+1/2,qk+1)n_k \in [q_{k+1}/2, q_{k+1}) with Matchs(nk ⁣+ ⁣1,qk)qk+1/16\operatorname{Match}{\mathbf{s}}(n_k!+!1, q_k) \ge q{k+1}/16. Define mk:=qk+1/16m_k := \lfloor q_{k+1}/16 \rfloor (truncating the match to a controlled length). The factor Uk:=snk+1snk+qk+mkU_k := s_{n_k+1} \cdots s_{n_k+q_k+m_k} has length k=qk+mkqk+qk+1(M ⁣+ ⁣2)qk\ell_k = q_k + m_k \le q_k + q_{k+1} \le (M!+!2),q_k (using qk+1(M ⁣+ ⁣1)qkq_{k+1} \le (M!+!1)q_k). By linear recurrence, R(k)(M ⁣+ ⁣2)k(M ⁣+ ⁣2)2qkR(\ell_k) \le (M!+!2),\ell_k \le (M!+!2)^2 q_k. So there exists an occurrence of UkU_k starting at some

rk[Aqk+1,  Aqk+1+(M ⁣+ ⁣2)2qk].r_k \in [Aq_{k+1},; Aq_{k+1} + (M!+!2)^2 q_k].

Set Nk:=F(rk)N_k := F(r_k) and Gk:=F(rk+qk)F(rk)G_k := F(r_k + q_k) - F(r_k). Since rkAqk+1+(M ⁣+ ⁣2)2qk(A+(M ⁣+ ⁣2)2)qk+1r_k \le Aq_{k+1} + (M!+!2)^2 q_k \le (A + (M!+!2)^2) q_{k+1}:

Nkλ(A+(M ⁣+ ⁣2)2)qk+1+B.N_k \le \lambda(A + (M!+!2)^2) q_{k+1} + B.

Also NkλAqk+1BN_k \ge \lambda A q_{k+1} - B and Gkλqk+2BG_k \le \lambda q_k + 2B, so for large kk,

GkNk    λqk+2BλAqk+1B    2A  <  1α,\frac{G_k}{N_k} ;\le; \frac{\lambda q_k + 2B}{\lambda A q_{k+1} - B} ;\le; \frac{2}{A} ;<; \frac{1}{\alpha},

since A>2αA > 2\alpha and qkqk+1q_k \le q_{k+1}. Also Gk3NkG_k \le 3N_k. Using the upper bound on NkN_k: Lklminmklminqk+1/32c2NkL_k \ge l_{\min}, m_k \ge l_{\min}, q_{k+1}/32 \ge c_2 N_k where c2:=lmin/(64λ(A+(M ⁣+ ⁣2)2))>0c_2 := l_{\min}/(64\lambda(A + (M!+!2)^2)) > 0.

Conclusion (both cases). In both cases, we obtain an infinite sequence of (Nk,Gk)(N_k, G_k) with Gk3NkG_k \le 3N_k, a digit match of length Lkc0NkL_k \ge c_0 N_k for a fixed constant c0>0c_0 > 0 (independent of kk), and additionally: in Case A with α2\alpha\ge 2 and in Case B, we have Gk(1+ε)Nk/αG_k \le (1+\varepsilon) N_k/\alpha for small ε>0\varepsilon>0.

Let K1,kK_{1,k} and K2,kK_{2,k} be the epoch indices of NkN_k and Nk+GkN_k + G_k, and set dk:=K2,kK1,kd_k := K_{2,k} - K_{1,k}. If dk=0d_k = 0 (same epoch), Theorem 4.1 gives M(Nk,Gk)K1,kα+Cwe=O(Nk)M(N_k, G_k) \le K_{1,k}\alpha + C_{\mathrm{we}} = O(\sqrt{N_k}). If dk1d_k \ge 1, we verify dkD(K1,k)d_k\le D(K_{1,k}). Since Gk3NkG_k \le 3N_k, we have Nk+Gk4Nk<4(K1,k ⁣+ ⁣1)2N_k + G_k \le 4N_k < 4(K_{1,k}!+!1)^2, so K2,k<2(K1,k ⁣+ ⁣1)K_{2,k} < 2(K_{1,k}!+!1) and

dkK1,k+1K1,k+2.d_k \le K_{1,k} + 1 \le K_{1,k} + 2.

In Case A with α<2\alpha<2: D(K1,k)=K1,k+2D(K_{1,k})=K_{1,k}+2, so the above gives dkD(K1,k)d_k\le D(K_{1,k}) directly.

In Case A with α2\alpha\ge 2 and in Case B: since Nk+GkN_k + G_k lies in epoch K2,kK_{2,k},

Gk    K2,k2(K1,k ⁣+ ⁣1)2+1  =  2K1,k(dk ⁣ ⁣1)+dk2,G_k ;\ge; K_{2,k}^2 - (K_{1,k}!+!1)^2 + 1 ;=; 2K_{1,k}(d_k!-!1) + d_k^2,

hence dk1+Gk/(2K1,k)d_k \le 1 + G_k/(2K_{1,k}). Since Gk(1+ε)Nk/α<(1+ε)(K1,k ⁣+ ⁣1)2/αG_k \le (1+\varepsilon) N_k/\alpha < (1+\varepsilon)(K_{1,k}!+!1)^2/\alpha,

dk    1+(1+ε)(K1,k+1)22αK1,k    2K1,k+2αd_k ;\le; 1 + \frac{(1+\varepsilon)(K_{1,k}+1)^2}{2\alpha K_{1,k}} ;\le; \frac{2K_{1,k}+2}{\alpha}

for ε\varepsilon small and kk large. Thus dkD(K1,k)d_k \le D(K_{1,k}).

In all sub-cases, Proposition 4.2 gives M(Nk,Gk)CNkM(N_k, G_k) \le C\sqrt{N_k}.

In either case,

c0Nk    Lk    M(Nk,Gk)    CNk,c_0 N_k ;\le; L_k ;\le; M(N_k, G_k) ;\le; C\sqrt{N_k},

so Nk(C/c0)2N_k \le (C/c_0)^2. This contradicts NkN_k \to \infty.

The contradiction proves Theorem 1.1. ∎


6. Proof of Theorem 1.2

For the quantitative theorem we count factors that are completely contained in their starting epochs. This avoids the local restriction in Proposition 4.2.

Lemma 6.1 (Cross-epoch separation for internal factors). Let n1n\ge 1, and let N1<N2N_1<N_2 lie in epochs K1<K2K_1<K_2 with K11K_1\ge 1. Suppose that the orbit points decompose as zNi=Pi/cKi+Tiz_{N_i}=P_i/c^{K_i}+T_i with gcd(Pi,c)=1\gcd(P_i,c)=1 and

TiCtailcKi+1beNi(i=1,2)T_i\le \frac{C_{\mathrm{tail}}}{c^{K_i+1},b^{e_{N_i}}} \qquad (i=1,2)

for some constant Ctail1C_{\mathrm{tail}}\ge 1 satisfying 4Ctail<bc24C_{\mathrm{tail}}< bc^2. Assume

eN1n,eN2n,e_{N_1}\ge n,\qquad e_{N_2}\ge n,

and also

nαK2+1.n\ge \alpha K_2+1.

Then

zN1zN212cK2.|z_{N_1}-z_{N_2}|\ge \frac{1}{2c^{K_2}}.

Consequently,

M(N1,N2N1)K2α+logb2.M(N_1,N_2-N_1)\le K_2\alpha+\log_b 2.

Proof. Set

δ:=K2K11,D:=cδP1P2.\delta:=K_2-K_1\ge 1, \qquad D:=c^\delta P_1-P_2.

Then cDc\nmid D because ccδP1c\mid c^\delta P_1 and cP2c\nmid P_2. Hence D0D\ne 0 and

DcK21cK2.\left|\frac{D}{c^{K_2}}\right|\ge \frac{1}{c^{K_2}}.

Also

zN1zN2=DcK2+(T1T2).z_{N_1}-z_{N_2}=\frac{D}{c^{K_2}}+(T_1-T_2).

By the tail hypothesis and eNine_{N_i}\ge n,

TiCtailcKi+1bn(i=1,2).T_i\le \frac{C_{\mathrm{tail}}}{c^{K_i+1}b^n} \qquad (i=1,2).

For T1T_1, using δ1K22\delta-1\le K_2-2 (since K11K_1\ge 1) and nαK2+1n\ge \alpha K_2+1,

1cK1+1bn=1cK2bα(δ1)n1cK2bα(K22)n1bc21cK2.\frac{1}{c^{K_1+1}b^n} = \frac{1}{c^{K_2}},b^{\alpha(\delta-1)-n} \le \frac{1}{c^{K_2}},b^{\alpha(K_2-2)-n} \le \frac{1}{bc^2},\frac{1}{c^{K_2}}.

For T2T_2,

1cK2+1bn1cK2+1bαK2+1=1bc2K2+11bc21cK2.\frac{1}{c^{K_2+1}b^n} \le \frac{1}{c^{K_2+1}b^{\alpha K_2+1}} = \frac{1}{bc^{2K_2+1}} \le \frac{1}{bc^2},\frac{1}{c^{K_2}}.

Therefore

T1T2T1+T22Ctailbc21cK2.|T_1-T_2| \le T_1+T_2 \le \frac{2C_{\mathrm{tail}}}{bc^2},\frac{1}{c^{K_2}}.

Since 4Ctail<bc24C_{\mathrm{tail}}<bc^2,

2Ctailbc2<12.\frac{2C_{\mathrm{tail}}}{bc^2}<\frac12.

Thus

T1T2<12cK2.|T_1-T_2|<\frac{1}{2c^{K_2}}.

Together with the lattice gap, this yields

zN1zN21cK212cK2=12cK2.|z_{N_1}-z_{N_2}| \ge \frac{1}{c^{K_2}}-\frac{1}{2c^{K_2}} = \frac{1}{2c^{K_2}}.

The match bound follows from (5). ∎

Proof of Theorem 1.2. Let KweK_{\mathrm{we}} and CweC_{\mathrm{we}} be as in Theorem 4.1, and define

C:=max{Cwe,logb2}+2.C_*:=\max{C_{\mathrm{we}},\log_b 2}+2.

For n1n\ge 1, set

An:=n12,Bn:=nCα.A_n:=\left\lceil\frac{n-1}{2}\right\rceil, \qquad B_n:=\left\lfloor\frac{n-C_*}{\alpha}\right\rfloor.

Since α<2\alpha<2, we have

BnAn+1(1α12)n=2α2αn,B_n-A_n+1\sim \left(\frac{1}{\alpha}-\frac12\right)n = \frac{2-\alpha}{2\alpha},n,

so in particular there exists n0=n0(b,c)n_0=n_0(b,c) such that for all nn0n\ge n_0,

AnKwe,BnAn,A_n\ge K_{\mathrm{we}}, \qquad B_n\ge A_n,

and

Rn:=BnAn+12α4αn.R_n:=B_n-A_n+1\ge \frac{2-\alpha}{4\alpha},n.

Fix nn0n\ge n_0. For each epoch K[An,Bn]K\in [A_n,B_n], let

NK(n):={NZ:K2N(K+1)2n}.\mathcal{N}_K(n):= {,N\in \mathbb{Z} : K^2\le N\le (K+1)^2-n,}.

Any length-nn factor starting at NNK(n)N\in\mathcal{N}_K(n) is fully contained in epoch KK, because then eNne_N\ge n. The number of such starting positions is

mK:=#NK(n)=(K+1)2nK2+1=2K+2n.m_K:=#\mathcal{N}_K(n) = (K+1)^2-n-K^2+1 = 2K+2-n.

We claim that all factors arising from

K=AnBnNK(n)\bigcup_{K=A_n}^{B_n}\mathcal{N}_K(n)

are pairwise distinct.

Same epoch. Let N1<N2N_1<N_2 lie in the same NK(n)\mathcal{N}_K(n), and set s:=N2N1s:=N_2-N_1. Then

1s(K+1)2nK2=2K+1n2K+1.1\le s\le (K+1)^2-n-K^2=2K+1-n\le 2K+1.

By Theorem 4.1,

M(N1,s)Kα+Cwe.M(N_1,s)\le K\alpha+C_{\mathrm{we}}.

Since KBnK\le B_n,

Kα+CwenC+Cwe<n.K\alpha+C_{\mathrm{we}} \le n-C_*+C_{\mathrm{we}}<n.

Hence the two length-nn factors are distinct.

Different epochs. Let N1NK1(n)N_1\in\mathcal{N}{K_1}(n) and N2NK2(n)N_2\in\mathcal{N}{K_2}(n) with K1<K2K_1<K_2. Then eN1ne_{N_1}\ge n and eN2ne_{N_2}\ge n by construction. Also K2BnK_2\le B_n, so

αK2+1nC+1<n.\alpha K_2+1\le n-C_*+1<n.

By (3), Lemma 3.1 gives the decomposition with Ctail=16/15C_{\mathrm{tail}}=16/15, and 416/15=64/15<8bc24\cdot 16/15=64/15<8\le bc^2. Thus Lemma 6.1 applies and gives

M(N1,N2N1)K2α+logb2nC+logb2<n.M(N_1,N_2-N_1)\le K_2\alpha+\log_b2\le n-C_*+\log_b2<n.

Hence these length-nn factors are also distinct.

Therefore

p(γb,c,b,n)K=AnBnmK.p(\gamma_{b,c},b,n)\ge \sum_{K=A_n}^{B_n} m_K.

Using the formula for mKm_K,

K=AnBnmK=K=AnBn(2K+2n)=Rn(An+Bn+2n).\sum_{K=A_n}^{B_n} m_K = \sum_{K=A_n}^{B_n}(2K+2-n) = R_n(A_n+B_n+2-n).

Now

An+Bn+2nRn=An+Bn+2n(BnAn+1)=2An+1n0,A_n+B_n+2-n-R_n = A_n+B_n+2-n-(B_n-A_n+1) = 2A_n+1-n\ge 0,

because An=(n1)/2A_n=\lceil(n-1)/2\rceil. Hence

An+Bn+2nRn,A_n+B_n+2-n\ge R_n,

and therefore

p(γb,c,b,n)Rn2.p(\gamma_{b,c},b,n)\ge R_n^2.

By the lower bound on RnR_n,

p(γb,c,b,n)(2α4αn)2=(2α)216α2n2.p(\gamma_{b,c},b,n) \ge \left(\frac{2-\alpha}{4\alpha},n\right)^2 = \frac{(2-\alpha)^2}{16\alpha^2},n^2.

This proves the theorem. ∎


7. A general epoch-expansion theorem

The proofs for γb,c\gamma_{b,c} and Md,b,cM_{d,b,c} share a common structure that applies to a wide class of lacunary constants. We now state and prove the general result announced in Theorem 1.5.

Proof of Theorem 1.5. Write α=logbc\alpha=\log_b c. For nn in epoch KK (i.e. f(K)n<f(K ⁣+ ⁣1)f(K)\le n<f(K!+!1)), the orbit point zn={bnξ}z_n={b^n\xi} decomposes as

zn  =  Pncg(K)+Tn,(10)z_n;=;\frac{P_n}{c^{g(K)}}+T_n, \tag{10}

where PnaKbnf(K)(modc)P_n\equiv a_K b^{n-f(K)}\pmod{c}, hence gcd(Pn,c)=1\gcd(P_n,c)=1 (since gcd(aK,c)=gcd(b,c)=1\gcd(a_K,c)=\gcd(b,c)=1), and TnCtail/(cg(K)+1bf(K+1)n)T_n\le C_{\mathrm{tail}}/(c^{g(K)+1}b^{f(K+1)-n}) for a constant CtailC_{\mathrm{tail}} depending only on b,cb,c (the geometric tail bound uses g(K ⁣+ ⁣1)g(K)+1g(K!+!1)\ge g(K)+1, which follows from gg strictly increasing, and f(K ⁣+ ⁣2)f(K ⁣+ ⁣1)f(K!+!2)-f(K!+!1)\to\infty). This is the direct analogue of Lemma 3.1 with cKc^K replaced by cg(K)c^{g(K)}, and k2k^2 replaced by f(k)f(k).

Within-epoch match bound. For n,n+sn,n+s in the same epoch KK with 1sLK1\le s\le L_K, the cc-adic valuation argument of Theorem 4.1 gives

M(n,s)    g(K)α+C0,(11)M(n,s);\le; g(K)\alpha+C_0, \tag{11}

provided vc(bs1)<g(K)v_c(b^s-1)<g(K), which holds for all sLKs\le L_K and all large KK by hypothesis (1).

Cross-epoch separation. For N1N_1 in epoch K1K_1 and N2N_2 in epoch K2>K1K_2>K_1 with f(Ki+1)Ninf(K_i+1)-N_i\ge n, the lattice gap D/cg(K2)1/cg(K2)|D/c^{g(K_2)}|\ge 1/c^{g(K_2)} (from cDc\nmid D exactly as in Lemma 6.1) dominates the tail difference whenever ng(K2)α+1n\ge g(K_2)\alpha+1.

Quantitative bound. For each epoch KK, the set NK(n)={N:f(K)Nf(K ⁣+ ⁣1)n}\mathcal{N}K(n)={N: f(K)\le N\le f(K!+!1)-n} has mK=LKn+1m_K=L_K-n+1 elements whenever LKnL_K\ge n. All length-nn factors from starting positions in K=AnBnNK(n)\bigcup{K=A_n}^{B_n}\mathcal{N}K(n) are pairwise distinct: same-epoch pairs are separated by (11) (using g(K)α+C0<ng(K)\alpha+C_0<n for KBnK\le B_n), and cross-epoch pairs by the lattice gap. Hence p(ξ,b,n)K=AnBn(LKn+1)p(\xi,b,n)\ge \sum{K=A_n}^{B_n}(L_K-n+1).

Qualitative statement. When the quantitative range is nonempty (i.e. BnAnB_n \ge A_n for all large nn), the divergence of the sum K=AnBn(LKn+1)\sum_{K=A_n}^{B_n}(L_K-n+1) gives p(ξ,b,n)np(\xi,b,n)-n\to\infty directly. This covers all cases where α<2\alpha < 2, and more generally whenever ff grows fast enough that Bn>AnB_n > A_n eventually.

When Bn<AnB_n < A_n (which can happen for polynomial ff with α2\alpha \ge 2), we use the Cassaigne argument of Theorem 1.1, with g(K)g(K) replacing KK. Assume for contradiction that lim inf(p(n)n)<\liminf(p(n)-n)<\infty. By Cassaigne's theorem, the digit sequence is eventually quasi-Sturmian. The within-epoch match bound (11) gives M(n,s)g(K)α+C0M(n,s)\le g(K)\alpha + C_0 for all gaps ss within epoch KK. Since g(K)=o(f(K))g(K) = o(f(K)) and LKL_K\to\infty, large epochs contain LK\gg L_K digit positions, and the quasi-Sturmian self-match of length Ω(N)\Omega(N) (from the Sturmian convergents, placed inside a single epoch as in Section 5) gives Ω(N)g(K)α+C0\Omega(N) \le g(K)\alpha + C_0. But g(K)α=o(N)g(K)\alpha = o(N) (since Nf(K)N \ge f(K) and g=o(f)g = o(f)), so Ω(N)=o(N)\Omega(N) = o(N), a contradiction. ∎

The following corollaries illustrate the scope of Theorem 1.5.

Corollary 7.1 (Polynomial exponents). Let r2r\ge 2 be an integer, b,c2b,c\ge 2 with gcd(b,c)=1\gcd(b,c)=1, and α=logbc\alpha=\log_b c. For any integers aka_k with gcd(ak,c)=1\gcd(a_k,c)=1, set ξ=k1ak/(ckbkr)\xi=\sum_{k\ge 1}a_k/(c^k b^{k^r}). Then:

(a) p(ξ,b,n)n+p(\xi,b,n)-n\to+\infty;

(b) if r=2r=2 and α<2\alpha<2, then p(ξ,b,n)c0n2p(\xi,b,n)\ge c_0,n^2 with c0=(2α)2/(16α2)c_0=(2-\alpha)^2/(16\alpha^2) (recovering Theorem 1.2);

(c) for r3r\ge 3 and any α>0\alpha>0, there exists cr>0c_r>0 such that p(ξ,b,n)crnrp(\xi,b,n)\ge c_r, n^r.

Proof. Take f(k)=krf(k)=k^r, g(k)=kg(k)=k. Then ff and gg are strictly increasing, LK=(K ⁣+ ⁣1)rKrrKr1L_K=(K!+!1)^r-K^r\sim rK^{r-1}, and g(K)=Kg(K)=K. Since logLK=O(logK)=o(K)=o(g(K))\log L_K = O(\log K) = o(K) = o(g(K)), hypothesis (1) is satisfied. In the quantitative bound, An(n/r)1/(r1)A_n\sim (n/r)^{1/(r-1)} and Bnn/αB_n\sim n/\alpha, so K=AnBn(LKn+1)cKn/αrKr1crnr\sum_{K=A_n}^{B_n}(L_K-n+1)\ge c\sum_{K\sim n/\alpha}rK^{r-1}\ge c_r n^r. For r=2r=2 this specializes to the quadratic bound of Theorem 1.2. For r3r\ge 3, Bnn/αB_n\sim n/\alpha regardless of whether α<2\alpha<2, so no restriction on α\alpha is needed. When r=2r=2 and α2\alpha \ge 2, the quantitative range is empty (Bn<AnB_n < A_n), but the qualitative conclusion p(n)np(n)-n\to\infty follows from the Cassaigne argument in the proof of Theorem 1.5. ∎

Corollary 7.2 (Exponential exponents). Let d2d\ge 2, b,c2b,c\ge 2 with gcd(b,c)=1\gcd(b,c)=1 and d<cd<c. Then Md,b,c=k01/(ckbdk)M_{d,b,c}=\sum_{k\ge 0}1/(c^k b^{d^k}) satisfies p(Md,b,c,b,n)dn/αCp(M_{d,b,c},b,n)\ge d^{n/\alpha-C} (recovering Theorem 1.4).

Proof. Take f(k)=dkf(k)=d^k, g(k)=kg(k)=k. Then ff and gg are strictly increasing, LK=(d ⁣ ⁣1)dKL_K=(d!-!1)d^K, and g(K)=Kg(K)=K. Here logLKKlogd\log L_K \sim K\log d, so the sufficient condition logLK=o(g(K))\log L_K = o(g(K)) does not hold. Instead, hypothesis (1) is verified directly: since d<cd < c, the multiplicative order estimate (8) gives ordcK(b)>LK\operatorname{ord}_{c^K}(b) > L_K for large KK, hence vc(bs1)<K=g(K)v_c(b^s-1) < K = g(K) for all 1sLK1\le s \le L_K. The quantitative bound then gives AnlogdnA_n\sim\log_d n, Bnn/αB_n\sim n/\alpha, and the geometric sum yields p(n)dBn/2dn/αCp(n)\ge d^{B_n}/2\ge d^{n/\alpha-C}. ∎

Corollary 7.3 (Tschakaloff function values). For b,c2b,c\ge 2 with gcd(b,c)=1\gcd(b,c)=1, the Tschakaloff value

Tb(1/c)  =  k11ckbk(k+1)/2T_b(1/c);=;\sum_{k\ge 1}\frac{1}{c^k,b^{k(k+1)/2}}

satisfies p(Tb(1/c),b,n)n+p(T_b(1/c),b,n)-n\to+\infty. If α=logbc<2\alpha=\log_b c<2, then p(Tb(1/c),b,n)c0n2p(T_b(1/c),b,n)\ge c_0,n^2.

Proof. Take f(k)=k(k+1)/2f(k)=k(k+1)/2, g(k)=kg(k)=k. Then ff and gg are strictly increasing, LK=K+1L_K=K+1, and logLK=O(logK)=o(K)=o(g(K))\log L_K = O(\log K) = o(K) = o(g(K)), so hypothesis (1) holds. The spacing matches the quadratic case (ff is degree 2 in kk). ∎

Corollary 7.4 (Fibonacci-exponent constants). Let FkF_k denote the kk-th Fibonacci number and φ=(1+5)/2\varphi=(1+\sqrt{5})/2 the golden ratio. For b,c2b,c\ge 2 with gcd(b,c)=1\gcd(b,c)=1 and φ<c\varphi<c, the constant ξ=k11/(ckbFk)\xi=\sum_{k\ge 1}1/(c^k b^{F_k}) satisfies p(ξ,b,n)φn/αCp(\xi,b,n)\ge \varphi^{n/\alpha-C} for a constant C=C(b,c)C=C(b,c).

Proof. Take f(k)=Fkf(k)=F_k, g(k)=kg(k)=k. Then ff and gg are strictly increasing, LK=FK+1FK=FK1φK1/5L_K=F_{K+1}-F_K=F_{K-1}\sim \varphi^{K-1}/\sqrt{5} (exponential growth at rate φ\varphi). As in Corollary 7.2, logLKKlogφ\log L_K \sim K\log\varphi is not o(g(K))o(g(K)), so hypothesis (1) is verified via multiplicative orders: since φ<c\varphi<c, the argument of (8) (with dd replaced by φ\varphi) gives ordcK(b)\operatorname{ord}_{c^K}(b) exceeds LKL_K for large KK. The geometric sum gives p(n)φBnφn/αCp(n)\ge \varphi^{B_n}\ge \varphi^{n/\alpha-C}. ∎

Corollary 7.5 (Signed coefficients). Theorem 1.5 holds with ak{+1,1}a_k\in{+1,-1}. In particular, it covers values of the Rogers false theta function

F(x,y)  =  k0(1)kxk(k+1)/2ykF(x,y);=;\sum_{k\ge 0}(-1)^k x^{k(k+1)/2}y^k

at x=1/bx=1/b, y=1/cy=1/c: the constant ξ=k0(1)k/(ckbk(k+1)/2)\xi=\sum_{k\ge 0}(-1)^k/(c^k b^{k(k+1)/2}) satisfies p(ξ,b,n)n+p(\xi,b,n)-n\to+\infty.

Proof. Since gcd(±1,c)=1\gcd(\pm 1,c)=1 for all c2c\ge 2, the coprimality hypothesis gcd(ak,c)=1\gcd(a_k,c)=1 holds. The proof of Theorem 1.5 uses gcd(Pn,c)=1\gcd(P_n,c)=1 via PnaKbnf(K)(modc)P_n\equiv a_K b^{n-f(K)}\pmod{c}; this requires only gcd(aK,c)=1\gcd(a_K,c)=1 and gcd(b,c)=1\gcd(b,c)=1. ∎

Remark 7.6. Corollary 7.3 is, to our knowledge, the first digit complexity result for Tschakaloff function values. Corollary 7.4 gives a natural family where the exponent function ff grows at a non-integer exponential rate φ\varphi.


8. The exponential case: twisted Mahler constants

For d2d\ge 2, b2b\ge 2, c2c\ge 2 with gcd(b,c)=1\gcd(b,c)=1, define

Md,b,c  :=  k01ckbdk.M_{d,b,c} ;:=; \sum_{k\ge 0}\frac{1}{c^k, b^{,d^k}}.

These are values of a twisted Mahler function ykxdk\sum y^k x^{d^k} at x=1/bx=1/b, y=1/cy=1/c (the factor yk=cky^k = c^{-k} twists the classical Mahler series xdk\sum x^{d^k}, introducing coprime denominators that fundamentally change the digit structure).

Remark 8.1 (Failure of prior methods). When d3d\ge 3 and c>d2c>d^2, both previously available approaches to proving p(n)np(n)-n\to\infty are provably inapplicable to Md,b,cM_{d,b,c}.

Diophantine method. Bugeaud and Kim [BK19] show that if μ(ξ)<μ0\mu(\xi)<\mu_0, where μ0=(25+410)/152.510\mu_0=(25+4\sqrt{10})/15\approx 2.510, then the initial repetition index of the base-bb expansion of ξ\xi exceeds 103/2\sqrt{10}-3/2, which is incompatible with quasi-Sturmian structure and forces p(n)np(n)-n\to\infty. Their argument requires the irrationality exponent to be strictly below μ0\mu_0 in order for the first link of the Adamczewski--Bugeaud chain [AB07] to produce the needed repetition bound. For Md,b,cM_{d,b,c} with d3d\ge 3 one has μ(Md,b,c)d3>μ0\mu(M_{d,b,c})\ge d\ge 3>\mu_0 (see below), so this chain breaks at the outset.

Hot spot method. Bailey--Crandall [BC02] prove normality of Md,b,cM_{d,b,c} when d>cd>\sqrt{c} (Corollary 4.9(iv) of [BC02]): their Theorem 4.8 requires μk/cγnk\mu_k/c^{\gamma n_k} to be nondecreasing for some γ>1/2\gamma>1/2, and for Md,b,cM_{d,b,c} one has μkdk\mu_k\sim d^k, nk=kn_k=k, so the condition holds iff d>cγd>c^{\gamma} for some γ>1/2\gamma>1/2, i.e. iff d>cd>\sqrt{c}. For Md,b,cM_{d,b,c}, epoch KK has length LK=(d1)dKL_K=(d-1)d^K and the relevant lattice denominator is cKc^K. When c>d2c>d^2, one has dcd\le\sqrt{c}, so the Bailey--Crandall condition fails.

Lower bound μ(Md,b,c)d\mu(M_{d,b,c})\ge d. The partial sum SN=k=0N11/(ckbdk)S_N=\sum_{k=0}^{N-1}1/(c^k b^{d^k}) has denominator dividing qN:=cN1bdN1q_N:=c^{N-1}b^{d^{N-1}}. The tail satisfies Md,b,cSN2/(cNbdN)|M_{d,b,c}-S_N|\le 2/(c^N b^{d^N}). For any w<dw<d, one has qNw1=O(b(w1)dN1)q_N^{w-1}=O(b^{(w-1)d^{N-1}}), while 1/Md,b,cSN=Ω(bdN)1/|M_{d,b,c}-S_N|=\Omega(b^{d^N}). Since (w1)dN1<dN(w-1)d^{N-1}<d^N for w<dw<d, it follows that Md,b,cSN<1/qNw|M_{d,b,c}-S_N|<1/q_N^w for all large NN, whence μd\mu\ge d. See Badziahin [Bad19] and Rajchert [Raj24] for the matching upper bound μ(Md,b,c)=d\mu(M_{d,b,c})=d.

Theorem 1.3 establishes p(n)np(n)-n\to\infty for all d2d\ge 2, including the regime d3d\ge 3, c>d2c>d^2 where both methods above are provably inapplicable. When d<cd<c, Theorem 1.4 strengthens this to the exponential bound p(Md,b,c,b,n)dn/αCp(M_{d,b,c},b,n)\ge d^{n/\alpha-C}, where α=logbc\alpha=\log_b c and C=C(d,b,c)C=C(d,b,c). Theorems 1.3 and 1.4 therefore provide, to our knowledge, the first exponential complexity bound for constants where both the Diophantine method and the hot spot method are provably inapplicable. The exponential growth rate dn/αd^{n/\alpha} is exponential in nn (specifically dn/α=bnlogbd/logbcd^{n/\alpha} = b^{n \log_b d / \log_b c}, which equals bn/2b^{n/2} when d=cd = \sqrt{c}); for comparison, the best quantitative bounds from the Bugeaud--Kim method yield only lim supp(n)/n4/3\limsup, p(n)/n \ge 4/3 [BKK25].

Proof of Theorem 1.3. Epoch structure. Epoch KK covers digit positions [dK,dK+1)[d^K, d^{K+1}), with length LK=(d1)dKL_K=(d-1)d^K. For nn in epoch KK, the orbit point decomposes as zn=Pn/cK+Tnz_n = P_n/c^K + T_n with gcd(Pn,c)=1\gcd(P_n,c)=1 and Tn2/(cK+1ben)T_n \le 2/(c^{K+1}b^{e_n}), where en=dK+1ne_n=d^{K+1}-n. To verify: bnMd,b,c=k0ckbndkb^n M_{d,b,c} = \sum_{k\ge 0} c^{-k}b^{n-d^k}; the k=0k=0 term bn1b^{n-1} is an integer, so zn={k1ckbndk}z_n = \bigl{\sum_{k\ge 1} c^{-k}b^{n-d^k}\bigr}. The finite part is Qn/cKQ_n/c^K with Qn=k=1KcKkbndkQ_n = \sum_{k=1}^{K} c^{K-k}, b^{n-d^k}. Set PnQncKP_n \equiv Q_n \bmod c^K; then PnbndK(modc)P_n \equiv b^{n-d^{K}} \pmod{c} (the k=Kk=K term; all earlier terms carry a factor of cc), so gcd(Pn,c)=1\gcd(P_n,c)=1 since gcd(b,c)=1\gcd(b,c)=1. The tail satisfies Tn=kK+1ckbndkc(K+1)beni0bi2/(cK+1ben)T_n = \sum_{k\ge K+1} c^{-k} b^{n-d^k} \le c^{-(K+1)}b^{-e_n}\sum_{i\ge 0} b^{-i} \le 2/(c^{K+1}b^{e_n}). The within-epoch match bound M(n,s)Kα+C0M(n,s)\le K\alpha+C_0 holds for any 1sLK1\le s\le L_K with vc(bs1)<Kv_c(b^s-1)<K, by the same valuation argument as Theorem 4.1. The key identities transfer directly: since both nn and n+sn+s lie in epoch KK, the tail sums Tn=kK+1ckbndkT_n=\sum_{k\ge K+1}c^{-k}b^{n-d^k} and Tn+s=kK+1ckbn+sdkT_{n+s}=\sum_{k\ge K+1}c^{-k}b^{n+s-d^k} involve the same future epochs kK+1k\ge K+1, so Tn+s=bsTnT_{n+s}=b^s T_n. The finite-part congruence Pn+sbsPn(modcK)P_{n+s}\equiv b^s P_n\pmod{c^K} likewise follows from Qn+s=bsQnQ_{n+s}=b^s Q_n. The hypothesis vc(bs1)<Kv_c(b^s-1)<K then gives vc(Δ)=vc(bs1)v_c(\Delta)=v_c(b^s-1), and the argument concludes as in Theorem 4.1.

Irrationality. The partial sums SN=k=0N1ckbdkS_N=\sum_{k=0}^{N-1}c^{-k}b^{-d^k} have denominator qN=cN1bdN1q_N=c^{N-1}b^{d^{N-1}} and satisfy Md,b,cSN2/(cNbdN)|M_{d,b,c}-S_N|\le 2/(c^N b^{d^N}), while qN+1/qN=cbdNdN1q_{N+1}/q_N=cb^{d^N-d^{N-1}}\to\infty; the same rational-approximation argument as Lemma 3.2 gives Md,b,cQM_{d,b,c}\notin\mathbb{Q}.

Contradiction. Assume lim inf(p(n)n)<\liminf(p(n)-n)<\infty. By Theorem 2.3, the digit sequence is eventually quasi-Sturmian: x=Wφ(s)\mathbf{x}=W\varphi(\mathbf{s}) with Sturmian slope β\beta, convergents qkq_k, and non-erasing morphism φ\varphi with lmin1l_{\min}\ge 1, lmax1l_{\max}\ge 1.

By Lemma 2.4, for large kk there exists nkn_k with Matchs(nk ⁣+ ⁣1,qk)qk+1/16\operatorname{Match}{\mathbf{s}}(n_k!+!1,q_k)\ge q{k+1}/16. Set k:=qk+1/16\ell_k:=\lfloor q_{k+1}/16 \rfloor. The Sturmian factor Uk:=snk+1snk+kU_k:=s_{n_k+1}\cdots s_{n_k+\ell_k} has length k\ell_k; the factor UkU_k also appears starting at position nk+qk+1n_k+q_k+1 (by the match of length k\ge\ell_k at gap qkq_k).

Target epoch. Choose K=max(logd(C1qk+1),  v0+1+logc(C2qk+1))K_*=\max(\lceil\log_d(C_1 q_{k+1})\rceil,; v_0+1+\lceil\log_c(C_2 q_{k+1})\rceil) where C1=16lmax/(d1)C_1=16l_{\max}/(d-1), C2=8lmax/d0C_2=8l_{\max}/d_0, d0=ordc(b)d_0=\operatorname{ord}c(b), v0=vc(bd01)v_0=v_c(b^{d_0}-1). Then K=O(logqk+1)K=O(\log q_{k+1}), the epoch length satisfies (d1)dK16lmaxqk+1(d-1)d^{K_}\ge 16l_{\max}q_{k+1}, and ordcK(b)8lmaxqk+1\operatorname{ord}{c^{K}}(b)\ge 8l_{\max}q_{k+1}. The order bound follows from the lifting-the-exponent lemma applied to each prime power pacp^a| c, combined via the Chinese remainder theorem: ordcK(b)cKv0/d0C2qk+1=8lmaxqk+1\operatorname{ord}{c^{K}}(b)\ge c^{K_*-v_0}/d_0\ge C_2 q_{k+1}=8l_{\max}q_{k+1} by the choice of KK_*; see (8) for the detailed calculation.

Two occurrences in one epoch. The first quarter of epoch KK_* spans (d1)dK/4(d-1)d^{K_*}/4 digit positions. Since each Sturmian letter maps to at most lmaxl_{\max} digits under φ\varphi, this corresponds to at least (d1)dK/(4lmax)4qk+1(d-1)d^{K_*}/(4l_{\max})\ge 4q_{k+1} Sturmian positions. Since R(k)2qk+1R(\ell_k)\le 2q_{k+1} (since k<qk+1\ell_k < q_{k+1} implies k[qj,qj+1)\ell_k \in [q_j, q_{j+1}) for some jkj \le k, giving R(k)qj+1+qj2qk+1R(\ell_k) \le q_{j+1} + q_j \le 2q_{k+1} by Lemma 2.5), splitting the window into two halves of 2qk+1\ge 2q_{k+1} positions yields two occurrences T0<T1T_0<T_1 of UkU_k. Both occurrences plus the factor stay inside epoch KK_*. Indeed, T1T_1 lies in the first quarter of epoch KK_*, so F(T1)dK+LK/4=dK+(d1)dK/4=(d+3)dK/4F(T_1)\le d^{K_*}+L_{K_*}/4=d^{K_*}+(d-1)d^{K_*}/4=(d+3)d^{K_*}/4. The factor length satisfies lmaxklmaxqk+1(d1)dK/16l_{\max}\ell_k\le l_{\max}q_{k+1}\le (d-1)d^{K_*}/16 by the choice of KK_*. Summing,

F(T1)+lmaxk    (d+3)4dK+(d1)16dK  =  4(d+3)+(d1)16dK  =  (5d+11)16dK.F(T_1)+l_{\max}\ell_k ;\le; \frac{(d+3)}{4},d^{K_*}+\frac{(d-1)}{16},d^{K_*} ;=; \frac{4(d+3)+(d-1)}{16},d^{K_*} ;=; \frac{(5d+11)}{16},d^{K_*}.

Since 5d+11<16d    11<11d    d>15d+11<16d\iff 11<11d\iff d>1, which holds for d2d\ge 2, we get F(T1)+lmaxk<dK+1F(T_1)+l_{\max}\ell_k<d^{K_*+1}.

Digit match and gap control. The identical factors at T0T_0 and T1T_1 produce a digit match of length Ldlminklminqk+1/32L_d\ge l_{\min}\ell_k\ge l_{\min}q_{k+1}/32 at gap g=F(T1)F(T0)g=F(T_1)-F(T_0). Since g4lmaxqk+1+O(1)g\le 4l_{\max}q_{k+1}+O(1) while ordcK(b)8lmaxqk+1\operatorname{ord}{c^{K}}(b)\ge 8l_{\max}q_{k+1} by the choice of KK_, we have g<ordcK(b)g<\operatorname{ord}{c^{K}}(b) once qk+1q_{k+1} exceeds a constant depending only on b,c,d,lmaxb,c,d,l_{\max}. Hence vc(bg1)<Kv_c(b^g-1)<K_, and the within-epoch bound gives

lminqk+132    Kα+C0  =  O(logqk+1).\frac{l_{\min}q_{k+1}}{32} ;\le; K_*\alpha+C_0 ;=; O(\log q_{k+1}).

This contradicts qk+1q_{k+1}\to\infty. ∎

Under the additional hypothesis d<cd<c we strengthen this to exponential growth (Theorem 1.4).

Remark 8.2. The condition d<cd<c is essential: it guarantees ordcK(b)cKv0/d0>LK=(d1)dK\operatorname{ord}{c^K}(b)\ge c^{K-v_0}/d_0>L_K=(d-1)d^K for all large KK (since (d/c)K0(d/c)^K\to 0), so that vc(bs1)<Kv_c(b^s-1)<K for every gap 1sLK1\le s\le L_K within epoch KK. When dcd\ge c, the multiplicative order can fall below the epoch length, creating gaps where the within-epoch match bound fails. In the μ\mu-bypass regime d3d\ge 3, c>d2c>d^2, the hypothesis d<cd<c is automatically satisfied. When d=2d = 2, one has μ(M2,b,c)=2<μ0\mu(M{2,b,c}) = 2 < \mu_0, so the Bugeaud--Kim method applies, yielding p(n)np(n)-n \to \infty by [BK19]; the contribution of Theorem 1.4 in this case is the explicit exponential growth rate, which the Diophantine method does not provide.

Proof of Theorem 1.4. Let C0C_0 be the constant from the within-epoch match bound (as in the proof of Theorem 1.3), and set C:=C0+logb2+2C_*:=C_0+\log_b 2+2.

Epoch parameters. Epoch KK covers digit positions [dK,dK+1)[d^K,d^{K+1}) with length LK=(d1)dKL_K=(d-1)d^K. Write d0:=ordc(b)d_0:=\operatorname{ord}_c(b) and v0:=vc(bd01)v_0:=v_c(b^{d_0}-1). Since d<cd<c, the ratio (d1)dKd0/cKv0=d0(d1)(d/c)Kcv00(d-1)d^K d_0/c^{K-v_0}=d_0(d-1)(d/c)^K c^{v_0}\to 0, so for all KK0K\ge K_0 (determined by b,c,db,c,d via d0d_0, v0v_0, and the inequality cKv0/d0>(d1)dKc^{K-v_0}/d_0>(d-1)d^K),

ordcK(b)cKv0d0>(d1)dK=LK.(8)\operatorname{ord}_{c^K}(b)\ge \frac{c^{K-v_0}}{d_0}>(d-1)d^K=L_K. \tag{8}

To see this: for each prime power pacp^a| c with dp:=ordp(b)d_p:=\operatorname{ord}p(b) and wp:=vp(bdp1)w_p:=v_p(b^{d_p}-1), the lifting-the-exponent lemma gives ordpaK(b)=dppa(K1)wp+a\operatorname{ord}{p^{aK}}(b)=d_p\cdot p^{a(K-1)-w_p+a} for KK large enough that aK>wpaK>w_p. Since gcd(b,c)=1\gcd(b,c)=1, the Chinese remainder theorem gives ordcK(b)=lcmp(ordpaK(b))cKv0/d0\operatorname{ord}_{c^K}(b)=\operatorname{lcm}p(\operatorname{ord}{p^{aK}}(b)) \ge c^{K-v_0}/d_0, where v0v_0 and d0d_0 absorb the finitely many prime-dependent constants. In particular, vc(bs1)<Kv_c(b^s-1)<K for every 1sLK1\le s\le L_K.

Usable epoch range. For a given factor length nn, define

Kmin:=logd ⁣(nd1),Kmax:=nCα.K_{\min}:=\left\lceil\log_d!\left(\frac{n}{d-1}\right)\right\rceil, \qquad K_{\max}:=\left\lfloor\frac{n-C_*}{\alpha}\right\rfloor.

If KKminK\ge K_{\min}, then LK=(d1)dKnL_K=(d-1)d^K\ge n, so any length-nn factor starting at position NN with eN:=dK+1Nne_N:=d^{K+1}-N\ge n is fully contained in epoch KK. If KKmaxK\le K_{\max}, then Kα+C0<n1<nK\alpha+C_0<n-1<n, so the within-epoch match bound forces any two positions in epoch KK at gap 1sLK1\le s\le L_K to produce distinct length-nn factors. Since Kmin=O(logn)K_{\min}=O(\log n) and Kmaxn/αK_{\max}\sim n/\alpha, the range [Kmin,Kmax][K_{\min},K_{\max}] is nonempty for all nn1n\ge n_1, where n1n_1 depends on b,c,db,c,d (via K0K_0, CC_*, and α\alpha).

Internal positions. For each K[Kmin,Kmax]K\in[K_{\min},K_{\max}], the set

NK(n):={NZ:dKNdK+1n}\mathcal{N}_K(n):={N\in\mathbb{Z}: d^K\le N\le d^{K+1}-n}

has cardinality mK=(d1)dKn+1m_K=(d-1)d^K-n+1. For KKmin+1K\ge K_{\min}+1 one has LKdn2nL_K\ge dn\ge 2n, so mKLK/2m_K\ge L_K/2.

Same-epoch distinctness. Let N1<N2NK(n)N_1<N_2\in\mathcal{N}_K(n) with s:=N2N1s:=N_2-N_1. Then 1sLK1\le s\le L_K. By (8), vc(bs1)<Kv_c(b^s-1)<K, so the within-epoch bound gives M(N1,s)Kα+C0<nM(N_1,s)\le K\alpha+C_0<n. Hence the two length-nn factors differ.

Cross-epoch distinctness. Let N1NK1(n)N_1\in\mathcal{N}{K_1}(n) and N2NK2(n)N_2\in\mathcal{N}{K_2}(n) with K1<K2KmaxK_1<K_2\le K_{\max}. Both positions satisfy eNine_{N_i}\ge n and K2α+1nC+1<nK_2\alpha+1\le n-C_*+1<n. The epoch decomposition (established above) gives zNi=Pi/cKi+Tiz_{N_i}=P_i/c^{K_i}+T_i with gcd(Pi,c)=1\gcd(P_i,c)=1 and Ti2/(cKi+1beNi)T_i\le 2/(c^{K_i+1}b^{e_{N_i}}), so the hypotheses of Lemma 6.1 hold with Ctail=2C_{\mathrm{tail}}=2 (and 42=8<bc24\cdot 2=8<bc^2 since gcd(b,c)=1\gcd(b,c)=1 forces bc212bc^2\ge 12). The lemma gives

M(N1,N2N1)K2α+logb2<n.M(N_1,N_2-N_1)\le K_2\alpha+\log_b 2<n.

Hence cross-epoch factors are also distinct.

Counting. All factors from K=KminKmaxNK(n)\bigcup_{K=K_{\min}}^{K_{\max}}\mathcal{N}_K(n) are pairwise distinct, so

p(Md,b,c,b,n)    K=KminKmaxmK    K=Kmin+1Kmax(d1)dK2.p(M_{d,b,c},b,n) ;\ge; \sum_{K=K_{\min}}^{K_{\max}} m_K ;\ge; \sum_{K=K_{\min}+1}^{K_{\max}}\frac{(d-1)d^K}{2}.

The geometric sum is dominated by its last term:

K=Kmin+1Kmax(d1)dK2  =  dKmax+1dKmin+12    dKmax2.\sum_{K=K_{\min}+1}^{K_{\max}}\frac{(d-1)d^K}{2} ;=; \frac{d^{K_{\max}+1}-d^{K_{\min}+1}}{2} ;\ge; \frac{d^{K_{\max}}}{2}.

Since Kmaxn/αC/α1K_{\max}\ge n/\alpha-C_*/\alpha-1, we obtain

p(Md,b,c,b,n)    12dn/αC/α1    dn/αCp(M_{d,b,c},b,n) ;\ge; \frac{1}{2},d^{,n/\alpha-C_*/\alpha-1} ;\ge; d^{,n/\alpha-C}

for all large nn, where C:=C/α+1+logd2C:=C_*/\alpha + 1 + \log_d 2 depends only on d,b,cd,b,c. ∎


9. Remarks and open questions

Remark 9.1 (Irrationality exponents). The arguments in this paper are completely independent of the irrationality exponents of γb,c\gamma_{b,c} and Md,b,cM_{d,b,c}. The method of [BK19] requires μ(ξ)<2.510\mu(\xi)<2.510\ldots; for comparison, μ(Md,b,c)d\mu(M_{d,b,c})\ge d for all d2d\ge 2, and the best known bound for π\pi is μ(π)7.103\mu(\pi)\le 7.103\ldots [ZZ20]. Our proofs avoid irrationality exponents entirely.

(1) Determine the exact growth order of p(γb,c,b,n)p(\gamma_{b,c},b,n). Is the quadratic lower bound in Theorem 1.2 close to optimal when α<2\alpha<2?

(2) Determine the irrationality exponent of γb,c\gamma_{b,c}.

(3) Theorem 1.4 gives an exponential bound when d<cd<c. Determine p(Md,b,c,b,n)p(M_{d,b,c},b,n) when dcd \ge c, and sharpen the base of the exponential.

(4) Investigate digit-distribution properties of γb,c\gamma_{b,c} and Md,b,cM_{d,b,c}, for example normality in base bb.

Remark 9.2 (Scope of the method). The epoch-expansion technique requires a lacunary series representation whose base and coefficient denominators are coprime, producing a single-modulus lattice that controls carry propagation. It does not apply to constants such as π\pi, log2\log 2, or 2\sqrt{2}, whose digit-generating iterations have dense perturbations and no single-modulus lattice structure. Whether the ideas of the present paper can be combined with other approaches to reach non-lacunary constants remains an open problem.


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