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The irrationality exponent of small-height binary lacunary series is 2

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

Let N≥2N\geq 2 be an integer and let λj\lambda_{j} be nonzero rational numbers with log⁡H⁢(λj)=o⁢(2j)\log H(\lambda_{j})=o(2^{j}), where H⁢(u/v)=max⁡(|u|,v)H(u/v)=\max(|u|,v) for u/vu/v in lowest terms with v>0v>0. We prove that ∑j≥0λj⁢N−2j\sum_{j\geq 0}\lambda_{j}N^{-2^{j}} is irrational and has irrationality exponent 22. The proof uses Padé approximants to the tails ∑r≥0λk+r⁢z2r\sum_{r\geq 0}\lambda_{k+r}z^{2^{r}}. The two Hankel families they need satisfy parity recursions, so they are nonzero for all nonzero weights. After the finite prefix of the series is cleared, the approximants of order nn give integer linear forms with height N(n+1/2)⁢2kN^{(n+1/2)2^{k}} and error N−(n+1/2)⁢2kN^{-(n+1/2)2^{k}}, up to factors eo⁢(2k)e^{o(2^{k})}. Only finitely many orders are used for each target exponent. The height condition cannot be weakened to log⁡H⁢(λj)≤C⁢2j\log H(\lambda_{j})\leq C2^{j} for any constant C>0C>0: for every CC some such weights give exponent greater than 22, and for larger CC positive integer weights can give a rational number or a Liouville number.

Key words and phrases:
irrationality exponent, lacunary series, rational height, Hankel determinant, Padé approximation
2020 Mathematics Subject Classification:
Primary 11J82; Secondary 11J70, 11B83

1. Introduction

For an irrational real number ξ\xi, its irrationality exponent is

μ⁢(ξ)=sup{ν∈ℝ:|ξ−pq|<q−ν⁢ for infinitely many ⁢(p,q)∈ℤ×ℤ>0}.\mu(\xi)=\sup\left\{\nu\in\mathbb{R}:\left|\xi-\frac{p}{q}\right|<q^{-\nu}% \text{ for infinitely many }(p,q)\in\mathbb{Z}\times\mathbb{Z}_{>0}\right\}.

The pigeonhole principle gives μ⁢(ξ)≥2\mu(\xi)\geq 2 (see the end of Section 5). Write L=log⁡NL=\log N. For a nonzero rational number in lowest terms, put

(1.1) H⁢(u/v)=max⁡(|u|,v),u∈ℤ∖{0},v∈ℤ>0,gcd⁡(u,v)=1.H(u/v)=\max(|u|,v),\qquad u\in\mathbb{Z}\setminus\{0\},\quad v\in\mathbb{Z}_{>% 0},\quad\gcd(u,v)=1.

We show that equality holds for binary lacunary series with rational weights of sufficiently small height.

Theorem 1.

Let N∈ℤN\in\mathbb{Z}, N≥2N\geq 2, and let (λj)j≥0(\lambda_{j})_{j\geq 0} be a sequence in ℚ∖{0}\mathbb{Q}\setminus\{0\} such that log⁡H⁢(λj)=o⁢(2j)\log H(\lambda_{j})=o(2^{j}). Then the absolutely convergent series

(1.2) x=∑j=0∞λj⁢N−2j=λ0N+λ1N2+λ2N4+λ3N8+⋯x=\sum_{j=0}^{\infty}\lambda_{j}N^{-2^{j}}=\frac{\lambda_{0}}{N}+\frac{\lambda% _{1}}{N^{2}}+\frac{\lambda_{2}}{N^{4}}+\frac{\lambda_{3}}{N^{8}}+\cdots

is irrational and satisfies μ⁢(x)=2\mu(x)=2.

Geometric weights λj=λj\lambda_{j}=\lambda^{j}, with λ∈ℚ∖{0}\lambda\in\mathbb{Q}\setminus\{0\}, satisfy the hypothesis because log⁡H⁢(λj)=O⁢(j)\log H(\lambda^{j})=O(j). Every sequence drawn in arbitrary order from a finite subset of ℚ∖{0}\mathbb{Q}\setminus\{0\} also satisfies the hypothesis, since its heights are bounded.

Duverney’s criterion [3, Corollary 3.4] already gives irrationality under this height condition. For wj=N2jw_{j}=N^{2^{j}}, its rationality exception would require

λj⁢λj+2=wj⁢λj+12\lambda_{j}\lambda_{j+2}=w_{j}\lambda_{j+1}^{2}

eventually. Here log⁡|λj⁢λj+2/λj+12|=o⁢(2j)\log|\lambda_{j}\lambda_{j+2}/\lambda_{j+1}^{2}|=o(2^{j}), whereas log⁡wj=2j⁢L\log w_{j}=2^{j}L, so the exception cannot occur. Duverney [3, Theorem 3.2] also studies finite exponent bounds. For related work, see his later paper [4].

Duverney, Kurosawa and Shiokawa [5, Theorem 1] consider signed series ∑ϵj/xj\sum\epsilon_{j}/x_{j}, where xj>1x_{j}>1 are rational and xj+1≥xj2x_{j+1}\geq x_{j}^{2} eventually. Their denominator condition is

(1.3) δ1=den⁡(x1),δj+1=δj2⁢den⁡(xj+1/xj2),log⁡δj+1=o⁢(log⁡xj),\delta_{1}=\operatorname{den}(x_{1}),\qquad\delta_{j+1}=\delta_{j}^{2}% \operatorname{den}(x_{j+1}/x_{j}^{2}),\qquad\log\delta_{j+1}=o(\log x_{j}),

where den\operatorname{den} is the reduced positive denominator. They conclude μ⁢(∑ϵj/xj)=lim supjlog⁡xj+1/log⁡xj\mu(\sum\epsilon_{j}/x_{j})=\limsup_{j}\log x_{j+1}/\log x_{j}. For xj=N2j/(t⁢|λj|)x_{j}=N^{2^{j}}/(t|\lambda_{j}|) with a fixed rational t>0t>0, the ratio is t⁢|λj|2/|λj+1|t|\lambda_{j}|^{2}/|\lambda_{j+1}|; the accumulated condition in (1.3) can fail even for a finite set of weights.

Amou and Bugeaud [1, Lemma 3] give an earlier criterion for ∑Bj/Aj\sum B_{j}/A_{j}, with strictly increasing positive integers AjA_{j} and nonzero integers BjB_{j}. Their hypotheses include ratios Sj=(Aj+1/|Bj+1|)/(Aj/|Bj|)2≥2S_{j}=(A_{j+1}/|B_{j+1}|)/(A_{j}/|B_{j}|)^{2}\geq 2 eventually and ∏r=0jdr2j−r=Ajo⁢(1)\prod_{r=0}^{j}d_{r}^{2^{j-r}}=A_{j}^{o(1)}, where dj=den⁡(Sj)d_{j}=\operatorname{den}(S_{j}) and d0=|B1|d_{0}=|B_{1}|; small heights alone do not imply this cumulative arithmetic condition.

For unit weights, Shallit [8, Theorems 8–9] proved bounded partial quotients when N≥3N\geq 3. For N=2N=2, he states the corresponding result for 2⁢∑j≥02−2j2\sum_{j\geq 0}2^{-2^{j}} [8, Theorem 11 and following example]. He also states a recursion for weights (−1)j(-1)^{j} when N≥3N\geq 3 [8, Theorem 12].

For nonzero integral geometric weights, Bugeaud, Han, Wen and Yao [2, Theorem 2.1] give exponent 22: g⁢(z)=∑r≥0λr⁢z2r−1g(z)=\sum_{r\geq 0}\lambda^{r}z^{2^{r}-1} has integer coefficients, satisfies g⁢(z)=1+λ⁢z⁢g⁢(z2)g(z)=1+\lambda zg(z^{2}), and has nonzero Hankel determinants of every order by Lemma 2.1. The multiplier λ⁢z\lambda z is nonzero on the orbit of 1/N1/N. The same theorem covers periodic rational weights. If the period is p≥1p\geq 1 and Dper∈ℤ>0D_{\mathrm{per}}\in\mathbb{Z}_{>0} clears the denominators, then f⁢(z)=Dper⁢∑j≥0λj⁢z2j−1∈ℤ⁢[[z]]f(z)=D_{\mathrm{per}}\sum_{j\geq 0}\lambda_{j}z^{2^{j}-1}\in\mathbb{Z}[[z]] converges in the unit disk and satisfies f⁢(z)=P⁢(z)+z2p−1⁢f⁢(z2p)f(z)=P(z)+z^{2^{p}-1}f(z^{2^{p}}) with P∈ℤ⁢[z]P\in\mathbb{Z}[z]. Lemma 2.1 gives every Hankel order, and z2p−1z^{2^{p}-1} does not vanish on the orbit of 1/N1/N. Since x=f⁢(1/N)/(Dper⁢N)x=f(1/N)/(D_{\mathrm{per}}N), [2, Theorem 2.1] gives μ⁢(x)=2\mu(x)=2. Su [9, Theorem 7.3] gives a formal continued fraction for ∑j≥0cj⁢z2j−1\sum_{j\geq 0}c_{j}z^{2^{j}-1} with c0=1c_{0}=1 and nonzero cjc_{j} in any field.

Rajchert [7] and Su [9] study related questions on irrationality exponents and continued fractions of Mahler-type series. None of our results depends on these works; apart from standard facts, every step is proved here.

For geometric weights, Mahler’s method also gives transcendence [6, Corollary 2]. The series F⁢(z)=∑r≥0λr⁢z2rF(z)=\sum_{r\geq 0}\lambda^{r}z^{2^{r}} has radius 11 and Hadamard gaps, so it is transcendental over ℂ⁢(z)\mathbb{C}(z). It satisfies F⁢(z)=z+λ⁢F⁢(z2)F(z)=z+\lambda F(z^{2}); the matrix of the system for (1,F⁢(z))𝖳(1,F(z))^{\mathsf{T}} and its inverse have polynomial entries. The orbit of 1/N1/N therefore contains no singular point.

Our proof uses moving tails and their Hankel recursions. After clearing the finite prefix, adjacent Padé approximants give integer pairs with nonzero determinant. For each target exponent the finite set of orders is fixed first, so all coefficient costs are o⁢(2k)o(2^{k}) at tail shift kk. Section 6 shows that the height scale is sharp.

Throughout the proof write

(1.4) λj=ujvj,uj∈ℤ∖{0},vj∈ℤ>0,gcd⁡(uj,vj)=1,hj=log⁡H⁢(λj).\begin{gathered}\lambda_{j}=\frac{u_{j}}{v_{j}},\qquad u_{j}\in\mathbb{Z}% \setminus\{0\},\quad v_{j}\in\mathbb{Z}_{>0},\quad\gcd(u_{j},v_{j})=1,\\ h_{j}=\log H(\lambda_{j}).\end{gathered}

In particular,

(1.5) e−hj≤|λj|≤ehj.e^{-h_{j}}\leq|\lambda_{j}|\leq e^{h_{j}}.

The upper bound and hj=o⁢(2j)h_{j}=o(2^{j}) give absolute convergence of (1.2). The moving tails are

(1.6) Fk⁢(z)=∑r≥0λk+r⁢z2r,Fk⁢(z)=λk⁢z+Fk+1⁢(z2).F_{k}(z)=\sum_{r\geq 0}\lambda_{k+r}z^{2^{r}},\qquad F_{k}(z)=\lambda_{k}z+F_{% k+1}(z^{2}).

For each fixed kk, the series converges absolutely for |z|<1|z|<1.

2. Hankel determinants

Put

(2.1) gk⁢(z)=Fk⁢(z)z=∑i≥0ai(k)⁢zi.g_{k}(z)=\frac{F_{k}(z)}{z}=\sum_{i\geq 0}a_{i}^{(k)}z^{i}.

By (1.6),

(2.2) a0(k)=λk,a2⁢i(k)=0(i≥1),a2⁢i+1(k)=ai(k+1)(i≥0).a_{0}^{(k)}=\lambda_{k},\qquad a_{2i}^{(k)}=0\quad(i\geq 1),\qquad a_{2i+1}^{(% k)}=a_{i}^{(k+1)}\quad(i\geq 0).

Define

(2.3) Hn(k)\displaystyle H_{n}^{(k)} =det(ai+j(k))0≤i,j<n,\displaystyle=\det(a_{i+j}^{(k)})_{0\leq i,j<n}, H0(k)\displaystyle H_{0}^{(k)} =1,\displaystyle=1,
Kn(k)\displaystyle K_{n}^{(k)} =det(ai+j+1(k))0≤i,j<n,\displaystyle=\det(a_{i+j+1}^{(k)})_{0\leq i,j<n}, K0(k)\displaystyle K_{0}^{(k)} =1.\displaystyle=1.
Lemma 2.1.

For all shifts k≥0k\geq 0, the determinants satisfy

(2.4) H2⁢m(k)\displaystyle H_{2m}^{(k)} =(−1)m⁢(Hm(k+1))2\displaystyle=(-1)^{m}(H_{m}^{(k+1)})^{2} (m≥1),\displaystyle(m\geq 1),
(2.5) H2⁢m+1(k)\displaystyle H_{2m+1}^{(k)} =(−1)m⁢λk⁢(Km(k+1))2\displaystyle=(-1)^{m}\lambda_{k}(K_{m}^{(k+1)})^{2} (m≥0),\displaystyle(m\geq 0),
(2.6) Kn(k)\displaystyle K_{n}^{(k)} =H⌈n/2⌉(k+1)⁢K⌊n/2⌋(k+1)\displaystyle=H_{\lceil n/2\rceil}^{(k+1)}K_{\lfloor n/2\rfloor}^{(k+1)} (n≥1).\displaystyle(n\geq 1).

In particular, Hn(k)⁢Kn(k)≠0H_{n}^{(k)}K_{n}^{(k)}\neq 0 for every n,k≥0n,k\geq 0.

Proof.

Ordering rows and columns by parity makes the two permutation signs cancel. For H2⁢m(k)H_{2m}^{(k)}, the matrix becomes

(λk⁢E00AA𝖳0),A=(ar+s(k+1))0≤r,s<m,\begin{pmatrix}\lambda_{k}E_{00}&A\\ A^{\mathsf{T}}&0\end{pmatrix},\qquad A=(a_{r+s}^{(k+1)})_{0\leq r,s<m},

where E00E_{00} has its sole nonzero entry 11 in the upper left corner. Exchanging the two blocks of mm columns contributes (−1)m2=(−1)m(-1)^{m^{2}}=(-1)^{m} and leaves diagonal blocks AA and A𝖳A^{\mathsf{T}}. This proves (2.4).

For H2⁢m+1(k)H_{2m+1}^{(k)}, separate index 0, the remaining even indices, and the odd indices. The case m=0m=0 gives H1(k)=λkH_{1}^{(k)}=\lambda_{k}. For m≥1m\geq 1, put

𝒂=(a0(k+1),…,am−1(k+1))𝖳,Gm=(ar+s+1(k+1))0≤r,s<m.\boldsymbol{a}=(a_{0}^{(k+1)},\ldots,a_{m-1}^{(k+1)})^{\mathsf{T}},\qquad G_{m% }=(a_{r+s+1}^{(k+1)})_{0\leq r,s<m}.

The matrix is

(2.7) (λk0𝒂𝖳00Gm𝒂Gm𝖳0).\begin{pmatrix}\lambda_{k}&0&\boldsymbol{a}^{\mathsf{T}}\\ 0&0&G_{m}\\ \boldsymbol{a}&G_{m}^{\mathsf{T}}&0\end{pmatrix}.

Since λk≠0\lambda_{k}\neq 0, pivoting on the first entry gives the Schur complement

(0GmGm𝖳−λk−1⁢𝒂⁢𝒂𝖳).\begin{pmatrix}0&G_{m}\\ G_{m}^{\mathsf{T}}&-\lambda_{k}^{-1}\boldsymbol{a}\boldsymbol{a}^{\mathsf{T}}% \end{pmatrix}.

For square blocks of size mm, column exchange gives

(2.8) det(0BCX)=(−1)m⁢detB⁢detC.\det\begin{pmatrix}0&B\\ C&X\end{pmatrix}=(-1)^{m}\det B\det C.

The determinant of (2.7) is (−1)m⁢λk⁢(detGm)2(-1)^{m}\lambda_{k}(\det G_{m})^{2}, proving (2.5).

For Kn(k)K_{n}^{(k)}, the mixed parity blocks vanish by (2.2). The diagonal blocks are

(ar+s(k+1))0≤r,s<⌈n/2⌉,(ar+s+1(k+1))0≤r,s<⌊n/2⌋.(a_{r+s}^{(k+1)})_{0\leq r,s<\lceil n/2\rceil},\qquad(a_{r+s+1}^{(k+1)})_{0% \leq r,s<\lfloor n/2\rfloor}.

This proves (2.6). Strong induction on nn, simultaneously for all kk, starts from

H0(k)=K0(k)=1,H1(k)=λk,K1(k)=λk+1.H_{0}^{(k)}=K_{0}^{(k)}=1,\qquad H_{1}^{(k)}=\lambda_{k},\qquad K_{1}^{(k)}=% \lambda_{k+1}.

Every remaining factor has smaller size, so all determinants are nonzero. ∎

Only offsets 0 and 11 are needed; other Hankel determinants may vanish, since a2(k)=0a_{2}^{(k)}=0. The weights may have either sign. For geometric weights, gk=λk⁢g0g_{k}=\lambda^{k}g_{0}; writing Hn=Hn(0)H_{n}=H_{n}^{(0)} and Kn=Kn(0)K_{n}=K_{n}^{(0)}, the recursions specialize to

H2⁢m=(−1)m⁢λ2⁢m⁢Hm2,H2⁢m+1=(−1)m⁢λ2⁢m⁢Km2,Kn=λn⁢H⌈n/2⌉⁢K⌊n/2⌋.H_{2m}=(-1)^{m}\lambda^{2m}H_{m}^{2},\qquad H_{2m+1}=(-1)^{m}\lambda^{2m}K_{m}% ^{2},\qquad K_{n}=\lambda^{n}H_{\lceil n/2\rceil}K_{\lfloor n/2\rfloor}.

3. Padé approximants to the moving tails

Lemma 3.1.

For each n≥1n\geq 1 and k≥0k\geq 0, there exist a positive integer dn,kd_{n,k} and polynomials Un,k,Vn,k∈ℤ⁢[z]U_{n,k},V_{n,k}\in\mathbb{Z}[z] with

(3.1) deg⁡Un,k,deg⁡Vn,k≤n,Vn,k⁢(0)=dn,k>0,\deg U_{n,k},\deg V_{n,k}\leq n,\qquad V_{n,k}(0)=d_{n,k}>0,

such that

(3.2) En,k⁢(z):=Vn,k⁢(z)⁢Fk⁢(z)−Un,k⁢(z)=cn,k⁢z2⁢n+1+O⁢(z2⁢n+2),cn,k∈ℤ∖{0}.E_{n,k}(z):=V_{n,k}(z)F_{k}(z)-U_{n,k}(z)=c_{n,k}z^{2n+1}+O(z^{2n+2}),\qquad c% _{n,k}\in\mathbb{Z}\setminus\{0\}.

They can be chosen so that, for each fixed finite set of orders, all their coefficients, dn,kd_{n,k} and |cn,k||c_{n,k}| are at most exp⁡(o⁢(2k))\exp(o(2^{k})), uniformly over that set as k→∞k\to\infty. They also satisfy the exact identity

(3.3) Un+1,k⁢Vn,k−Un,k⁢Vn+1,k=Ωn,k⁢z2⁢n+1,Ωn,k=dn+1,k⁢cn,k∈ℤ∖{0}.U_{n+1,k}V_{n,k}-U_{n,k}V_{n+1,k}=\Omega_{n,k}z^{2n+1},\qquad\Omega_{n,k}=d_{n% +1,k}c_{n,k}\in\mathbb{Z}\setminus\{0\}.
Proof.

Fix n,kn,k. By Lemma 2.1, the system

(3.4) ∑i=0n−1ai+j(k)⁢bi=−an+j(k)(0≤j<n)\sum_{i=0}^{n-1}a_{i+j}^{(k)}b_{i}=-a_{n+j}^{(k)}\qquad(0\leq j<n)

has a unique rational solution. For a power series WW, the notation [W]<n[W]_{<n} retains only powers below nn. Put

(3.5) pn,k⁢(T)=Tn+∑i=0n−1bi⁢Ti,Qn,k⁢(z)=zn⁢pn,k⁢(1/z),\displaystyle p_{n,k}(T)=T^{n}+\sum_{i=0}^{n-1}b_{i}T^{i},\qquad Q_{n,k}(z)=z^% {n}p_{n,k}(1/z),
(3.6) Pn,k⁢(z)=z⁢[Qn,k⁢(z)⁢gk⁢(z)]<n.\displaystyle P_{n,k}(z)=z[Q_{n,k}(z)g_{k}(z)]_{<n}.

Both polynomials have degree at most nn, and Qn,k⁢(0)=1Q_{n,k}(0)=1. Here [zℓ]⁢W[z^{\ell}]W denotes the coefficient of zℓz^{\ell} in WW.

Define the linear functional ℒk⁢(Tj)=aj(k)\mathcal{L}_{k}(T^{j})=a_{j}^{(k)}. For n≤ℓ<2⁢nn\leq\ell<2n, (3.4) gives

[zℓ]⁢(Qn,k⁢gk)=ℒk⁢(Tℓ−n⁢pn,k)=0.[z^{\ell}](Q_{n,k}g_{k})=\mathcal{L}_{k}(T^{\ell-n}p_{n,k})=0.

At ℓ=2⁢n\ell=2n, the bordered determinant formula gives

(3.7) ℒk⁢(Tn⁢pn,k)=a2⁢n(k)−𝒉𝖳⁢(ai+j(k))i,j<n−1⁢𝒉=Hn+1(k)Hn(k),𝒉=(an(k),…,a2⁢n−1(k))𝖳.\begin{split}\mathcal{L}_{k}(T^{n}p_{n,k})&=a_{2n}^{(k)}-\boldsymbol{h}^{% \mathsf{T}}(a_{i+j}^{(k)})_{i,j<n}^{-1}\boldsymbol{h}=\frac{H_{n+1}^{(k)}}{H_{% n}^{(k)}},\\ \boldsymbol{h}&=(a_{n}^{(k)},\ldots,a_{2n-1}^{(k)})^{\mathsf{T}}.\end{split}

Hence

(3.8) Qn,k⁢Fk−Pn,k=Hn+1(k)Hn(k)⁢z2⁢n+1+O⁢(z2⁢n+2).Q_{n,k}F_{k}-P_{n,k}=\frac{H_{n+1}^{(k)}}{H_{n}^{(k)}}z^{2n+1}+O(z^{2n+2}).

We choose the integerizer explicitly, because its size enters the height. Set

(3.9) ℓn=⌊log2⁡(2⁢n+1)⌋,𝒟n,k=∏r=0ℓnvk+r,Σn,k=∑r=0ℓnhk+r.\ell_{n}=\lfloor\log_{2}(2n+1)\rfloor,\qquad\mathcal{D}_{n,k}=\prod_{r=0}^{% \ell_{n}}v_{k+r},\qquad\Sigma_{n,k}=\sum_{r=0}^{\ell_{n}}h_{k+r}.

Every 𝒟n,k⁢ai(k)\mathcal{D}_{n,k}a_{i}^{(k)} with 0≤i≤2⁢n0\leq i\leq 2n is an integer. Let

(3.10) 𝔇n,k=det(𝒟n,k⁢ai+j(k))0≤i,j<n,dn,k=𝒟n,k⁢|𝔇n,k|.\mathfrak{D}_{n,k}=\det(\mathcal{D}_{n,k}a_{i+j}^{(k)})_{0\leq i,j<n},\qquad d% _{n,k}=\mathcal{D}_{n,k}|\mathfrak{D}_{n,k}|.

The determinant 𝔇n,k\mathfrak{D}_{n,k} is a nonzero integer. Cramer’s rule in (3.4) shows that every coefficient of dn,k⁢Qn,kd_{n,k}Q_{n,k} is an integer multiple of 𝒟n,k\mathcal{D}_{n,k}. Consequently

(3.11) Un,k=dn,k⁢Pn,k,Vn,k=dn,k⁢Qn,kU_{n,k}=d_{n,k}P_{n,k},\qquad V_{n,k}=d_{n,k}Q_{n,k}

are integer polynomials. The coefficient of degree 2⁢n+12n+1 in Vn,k⁢Fk−Un,kV_{n,k}F_{k}-U_{n,k} is also an integer: all coefficients of FkF_{k} needed at that degree have denominator dividing 𝒟n,k\mathcal{D}_{n,k}. By (3.8), it is

(3.12) cn,k=dn,k⁢Hn+1(k)Hn(k)≠0.c_{n,k}=d_{n,k}\frac{H_{n+1}^{(k)}}{H_{n}^{(k)}}\neq 0.

In particular, |cn,k|≥1|c_{n,k}|\geq 1.

Next we bound the sizes in Lemma 3.1. Write Σ=Σn,k\Sigma=\Sigma_{n,k}. Then

𝒟n,k≤eΣ,|𝒟n,k⁢ai(k)|≤e2⁢Σ(0≤i≤2⁢n).\mathcal{D}_{n,k}\leq e^{\Sigma},\qquad|\mathcal{D}_{n,k}a_{i}^{(k)}|\leq e^{2% \Sigma}\quad(0\leq i\leq 2n).

Expansion of the determinant, and of the integer Cramer numerators, gives

(3.13) 1≤|𝔇n,k|\displaystyle 1\leq|\mathfrak{D}_{n,k}| ≤n!⁢e2⁢n⁢Σ,\displaystyle\leq n!e^{2n\Sigma},
1≤dn,k\displaystyle 1\leq d_{n,k} ≤n!⁢e(2⁢n+1)⁢Σ,\displaystyle\leq n!e^{(2n+1)\Sigma},
max⁡{maxi⁡|[zi]⁢Un,k|,maxi⁡|[zi]⁢Vn,k|,|cn,k|}\displaystyle\max\left\{\max_{i}|[z^{i}]U_{n,k}|,\max_{i}|[z^{i}]V_{n,k}|,|c_{% n,k}|\right\} ≤(n+1)!⁢e(2⁢n+2)⁢Σ.\displaystyle\leq(n+1)!e^{(2n+2)\Sigma}.

For the last line, a coefficient of Un,kU_{n,k} or the leading error is a convolution of at most n+1n+1 terms; a coefficient of FkF_{k} contributes at most eΣe^{\Sigma}. The division by 𝔇n,k\mathfrak{D}_{n,k} cancels when the Cramer solution is multiplied by dn,kd_{n,k}. Since nn is fixed and hj=o⁢(2j)h_{j}=o(2^{j}), Σn,k=o⁢(2k)\Sigma_{n,k}=o(2^{k}), uniformly over finitely many orders. The polynomials, their integerizer and cn,kc_{n,k} depend only on the weights in (3.9); the remainder En,kE_{n,k} depends on the whole tail.

Finally, the polynomial on the left of (3.3) has degree at most 2⁢n+12n+1. Substituting Uj,k=Vj,k⁢Fk−Ej,kU_{j,k}=V_{j,k}F_{k}-E_{j,k} shows that it has no terms below degree 2⁢n+12n+1, and that the coefficient at that degree is dn+1,k⁢cn,k≠0d_{n+1,k}c_{n,k}\neq 0. Thus it is exactly the monomial in (3.3). ∎

We evaluate at a point that moves with kk. Put

(3.14) Δ=2k,y=N−Δ,εk=supj≥khj2j.\Delta=2^{k},\qquad y=N^{-\Delta},\qquad\varepsilon_{k}=\sup_{j\geq k}\frac{h_% {j}}{2^{j}}.

The hypothesis gives εk→0\varepsilon_{k}\to 0. Moreover,

(3.15) ∑j<khj=o⁢(2k).\sum_{j<k}h_{j}=o(2^{k}).

Given ρ>0\rho>0, choose JJ such that hj≤ρ⁢2jh_{j}\leq\rho 2^{j} for j≥Jj\geq J. The fixed sum before JJ, divided by 2k2^{k}, tends to zero, and the remaining sum divided by 2k2^{k} is at most ρ\rho.

Lemma 3.2.

For any fixed finite set of orders, uniformly over that set as k→∞k\to\infty,

(3.16) Qn,k⁢(y)\displaystyle Q_{n,k}(y) =1+O⁢(exp⁡(−L⁢Δ+o⁢(Δ))),\displaystyle=1+O\bigl{(}\exp(-L\Delta+o(\Delta))\bigr{)},
(3.17) En,k⁢(y)\displaystyle E_{n,k}(y) =cn,k⁢y2⁢n+1⁢(1+O⁢(exp⁡(−L⁢Δ+o⁢(Δ)))).\displaystyle=c_{n,k}y^{2n+1}\left(1+O\bigl{(}\exp(-L\Delta+o(\Delta))\bigr{)}% \right).

In particular, Vn,k⁢(y)>0V_{n,k}(y)>0 and En,k⁢(y)≠0E_{n,k}(y)\neq 0 for all sufficiently large kk, and

(3.18) log⁡|En,k⁢(y)|=−(2⁢n+1)⁢L⁢Δ+o⁢(Δ).\log|E_{n,k}(y)|=-(2n+1)L\Delta+o(\Delta).
Proof.

The integer Cramer numerators used above have absolute value at most n!⁢exp⁡(2⁢n⁢Σn,k)n!\exp(2n\Sigma_{n,k}), and their denominator is a nonzero integer. Thus the nonconstant coefficients of Qn,kQ_{n,k} have size exp⁡(o⁢(Δ))\exp(o(\Delta)). Since y=exp⁡(−L⁢Δ)y=\exp(-L\Delta), their finite sum proves (3.16). Also Vn,k=dn,k⁢Qn,kV_{n,k}=d_{n,k}Q_{n,k} with dn,k>0d_{n,k}>0, proving eventual positivity.

Fix nn, and split FkF_{k} after the terms with r≤ℓnr\leq\ell_{n}. The first omitted exponent is

tn=2ℓn+1>2⁢n+1.t_{n}=2^{\ell_{n}+1}>2n+1.

For every r≥0r\geq 0, the definition of εk\varepsilon_{k} gives

|λk+r|⁢y2r≤exp⁡(−(L−εk)⁢Δ⁢2r).|\lambda_{k+r}|y^{2^{r}}\leq\exp\bigl{(}-(L-\varepsilon_{k})\Delta 2^{r}\bigr{% )}.

For all sufficiently large kk, L−εk≥L/2L-\varepsilon_{k}\geq L/2 and

∑r≥ℓn+1|λk+r|⁢y2r\displaystyle\sum_{r\geq\ell_{n}+1}|\lambda_{k+r}|y^{2^{r}} ≤∑s≥0exp⁡(−(L−εk)⁢Δ⁢tn⁢2s)\displaystyle\leq\sum_{s\geq 0}\exp\bigl{(}-(L-\varepsilon_{k})\Delta t_{n}2^{% s}\bigr{)}
(3.19) ≤2⁢exp⁡(−(L−εk)⁢Δ⁢tn)=exp⁡(−L⁢tn⁢Δ+o⁢(Δ)).\displaystyle\leq 2\exp\bigl{(}-(L-\varepsilon_{k})\Delta t_{n}\bigr{)}=\exp(-% Lt_{n}\Delta+o(\Delta)).

The second inequality uses 2s≥s+12^{s}\geq s+1 and, for large kk, the geometric ratio exp⁡(−(L−εk)⁢Δ⁢tn)≤1/2\exp(-(L-\varepsilon_{k})\Delta t_{n})\leq 1/2.

Multiplying the finite part by Vn,kV_{n,k} and subtracting Un,kU_{n,k} gives a polynomial whose leading term is cn,k⁢z2⁢n+1c_{n,k}z^{2n+1}. All its subsequent terms have degree at least 2⁢n+22n+2 and coefficients of size exp⁡(o⁢(Δ))\exp(o(\Delta)) by (3.13). At yy, their sum is therefore at most exp⁡(−(2⁢n+2)⁢L⁢Δ+o⁢(Δ))\exp(-(2n+2)L\Delta+o(\Delta)). The omitted part, after multiplication by Vn,k⁢(y)V_{n,k}(y), is bounded by (3.19) with an additional factor exp⁡(o⁢(Δ))\exp(o(\Delta)). Since tn≥2⁢n+2t_{n}\geq 2n+2 and |cn,k|≥1|c_{n,k}|\geq 1, both parts, relative to cn,k⁢y2⁢n+1c_{n,k}y^{2n+1}, have absolute value at most exp⁡(−L⁢Δ+o⁢(Δ))\exp(-L\Delta+o(\Delta)). This proves (3.17), and the factor in parentheses is eventually nonzero. Finally, 0≤log⁡|cn,k|=o⁢(Δ)0\leq\log|c_{n,k}|=o(\Delta) proves (3.18); there are finitely many orders, so all bounds are uniform. ∎

4. Moving-tail iteration and integerization

Fix k≥1k\geq 1, so that NΔ/2N^{\Delta/2} below is an integer, and retain Δ=2k\Delta=2^{k}, y=N−Δy=N^{-\Delta}. Repeatedly splitting (1.6) gives the exact identity

(4.1) x=Sk+Fk⁢(y),Sk=∑j=0k−1ujvj⁢N2j.x=S_{k}+F_{k}(y),\qquad S_{k}=\sum_{j=0}^{k-1}\frac{u_{j}}{v_{j}N^{2^{j}}}.

Define

(4.2) Ck=lcm⁡(v0,…,vk−1),Tk=Ck⁢NΔ/2,Jk=Tk⁢Sk.C_{k}=\operatorname{lcm}(v_{0},\ldots,v_{k-1}),\qquad T_{k}=C_{k}N^{\Delta/2},% \qquad J_{k}=T_{k}S_{k}.

All three are integers: for j<kj<k, vjv_{j} divides CkC_{k} and 2j≤Δ/22^{j}\leq\Delta/2. Equations (3.15) and (4.2) give

(4.3) 0≤log⁡Ck≤∑j<khj=o⁢(Δ),log⁡Tk=12⁢L⁢Δ+o⁢(Δ).0\leq\log C_{k}\leq\sum_{j<k}h_{j}=o(\Delta),\qquad\log T_{k}=\tfrac{1}{2}L% \Delta+o(\Delta).

Put

(4.4) U~n,k\displaystyle\widetilde{U}_{n,k} =Nn⁢Δ⁢Un,k⁢(y),\displaystyle=N^{n\Delta}U_{n,k}(y), V~n,k\displaystyle\widetilde{V}_{n,k} =Nn⁢Δ⁢Vn,k⁢(y),\displaystyle=N^{n\Delta}V_{n,k}(y),
Bn,k\displaystyle B_{n,k} =Tk⁢V~n,k,\displaystyle=T_{k}\widetilde{V}_{n,k}, An,k\displaystyle A_{n,k} =Jk⁢V~n,k+Tk⁢U~n,k.\displaystyle=J_{k}\widetilde{V}_{n,k}+T_{k}\widetilde{U}_{n,k}.

The degree bounds give integer evaluations and hence integer pairs An,k,Bn,kA_{n,k},B_{n,k}. For all sufficiently large kk in a fixed finite order set, Bn,k>0B_{n,k}>0 and

(4.5) An,kBn,k\displaystyle\frac{A_{n,k}}{B_{n,k}} =Sk+Un,k⁢(y)Vn,k⁢(y),\displaystyle=S_{k}+\frac{U_{n,k}(y)}{V_{n,k}(y)},
(4.6) Bn,k⁢x−An,k\displaystyle B_{n,k}x-A_{n,k} =Tk⁢Nn⁢Δ⁢En,k⁢(y)≠0.\displaystyle=T_{k}N^{n\Delta}E_{n,k}(y)\neq 0.

Put

(4.7) τn,k=(n+12)⁢L⁢Δ.\tau_{n,k}=(n+\tfrac{1}{2})L\Delta.

Write the relative error in (3.17) as rn,k=o⁢(1)r_{n,k}=o(1). Then

(4.8) Bn,k\displaystyle B_{n,k} =Ck⁢dn,k⁢eτn,k⁢Qn,k⁢(y),\displaystyle=C_{k}d_{n,k}e^{\tau_{n,k}}Q_{n,k}(y),
(4.9) Bn,k⁢x−An,k\displaystyle B_{n,k}x-A_{n,k} =Ck⁢cn,k⁢e−τn,k⁢(1+rn,k).\displaystyle=C_{k}c_{n,k}e^{-\tau_{n,k}}(1+r_{n,k}).

Every additional logarithm in these two expressions is o⁢(Δ)o(\Delta), uniformly over a fixed finite set of orders. Hence

(4.10) log⁡Bn,k\displaystyle\log B_{n,k} =τn,k+o⁢(Δ),\displaystyle=\tau_{n,k}+o(\Delta),
(4.11) log⁡|Bn,k⁢x−An,k|\displaystyle\log|B_{n,k}x-A_{n,k}| =−τn,k+o⁢(Δ),\displaystyle=-\tau_{n,k}+o(\Delta),
(4.12) log⁡|x−An,kBn,k|\displaystyle\log\left|x-\frac{A_{n,k}}{B_{n,k}}\right| =−2⁢τn,k+o⁢(Δ).\displaystyle=-2\tau_{n,k}+o(\Delta).

The individual factors have logarithmic size

quantitylogarithmic size at fixed ⁢nTk12⁢L⁢Δ+o⁢(Δ)Nn⁢Δn⁢L⁢Δdn,k,|cn,k|o⁢(Δ)Vn,k⁢(y)o⁢(Δ)|En,k⁢(y)|−(2⁢n+1)⁢L⁢Δ+o⁢(Δ).\begin{array}[]{c|c}\text{quantity}&\text{logarithmic size at fixed }n\\ \hline\cr T_{k}&\frac{1}{2}L\Delta+o(\Delta)\\ N^{n\Delta}&nL\Delta\\ d_{n,k},\ |c_{n,k}|&o(\Delta)\\ V_{n,k}(y)&o(\Delta)\\ |E_{n,k}(y)|&-(2n+1)L\Delta+o(\Delta).\end{array}

The prefix costs 12⁢L⁢Δ\tfrac{1}{2}L\Delta, and the factor zz in Fk=z⁢gkF_{k}=zg_{k} raises the error order to 2⁢n+12n+1; the two halves balance, since 2⁢(n+12)=2⁢n+12(n+\tfrac{1}{2})=2n+1. Also |An,k|≤|x|⁢Bn,k+|Bn,k⁢x−An,k||A_{n,k}|\leq|x|B_{n,k}+|B_{n,k}x-A_{n,k}|, so An,kA_{n,k} obeys the same height bound.

The adjacent identity (3.3) gives

(4.13) An+1,k⁢Bn,k−An,k⁢Bn+1,k=Ck2⁢NΔ⁢Ωn,k≠0.A_{n+1,k}B_{n,k}-A_{n,k}B_{n+1,k}=C_{k}^{2}N^{\Delta}\Omega_{n,k}\neq 0.

The two terms containing JkJ_{k} cancel, leaving

Tk2⁢N(2⁢n+1)⁢Δ⁢(Un+1,k⁢(y)⁢Vn,k⁢(y)−Un,k⁢(y)⁢Vn+1,k⁢(y))\displaystyle T_{k}^{2}N^{(2n+1)\Delta}\bigl{(}U_{n+1,k}(y)V_{n,k}(y)-U_{n,k}(% y)V_{n+1,k}(y)\bigr{)}
=Ck2⁢N(2⁢n+2)⁢Δ⁢Ωn,k⁢y2⁢n+1=Ck2⁢NΔ⁢Ωn,k.\displaystyle\qquad=C_{k}^{2}N^{(2n+2)\Delta}\Omega_{n,k}y^{2n+1}=C_{k}^{2}N^{% \Delta}\Omega_{n,k}.

Hence, for every (p,q)∈ℤ×ℤ>0(p,q)\in\mathbb{Z}\times\mathbb{Z}_{>0}, the two integers

(4.14) Bn,k⁢p−q⁢An,k,Bn+1,k⁢p−q⁢An+1,kB_{n,k}p-qA_{n,k},\qquad B_{n+1,k}p-qA_{n+1,k}

cannot both vanish.

5. Proof of Theorem 1

First fix n=1n=1 and let k→∞k\to\infty. By (4.6) and (4.11), the forms B1,k⁢x−A1,kB_{1,k}x-A_{1,k} are eventually nonzero and tend to zero. If x=a/bx=a/b were rational, with a∈ℤa\in\mathbb{Z} and b∈ℤ>0b\in\mathbb{Z}_{>0}, then

b⁢(B1,k⁢x−A1,k)=B1,k⁢a−b⁢A1,kb(B_{1,k}x-A_{1,k})=B_{1,k}a-bA_{1,k}

would be a nonzero integer tending to zero, a contradiction. This proves irrationality.

For the upper bound we use a fixed finite set of orders. Fix an integer M≥1M\geq 1 and use primary orders M≤n≤2⁢MM\leq n\leq 2M, each with companion n+1n+1. The whole order set is therefore

(5.1) ℬ={M,M+1,…,2⁢M+1}.\mathcal{B}=\{M,M+1,\ldots,2M+1\}.

Put

(5.2) αM=1+1M+1/2.\alpha_{M}=1+\frac{1}{M+1/2}.

Order the primary scales τn,k\tau_{n,k} by increasing kk, and then increasing nn. This is their numerical order, because the largest scale in one block is (2⁢M+12)⁢L⁢2k(2M+\tfrac{1}{2})L2^{k}, and the first in the next is (2⁢M+1)⁢L⁢2k(2M+1)L2^{k}. Within a block, successive ratios are at most

M+3/2M+1/2=αM.\frac{M+3/2}{M+1/2}=\alpha_{M}.

At a block transition the ratio is

2⁢(M+1/2)2⁢M+1/2<αM.\frac{2(M+1/2)}{2M+1/2}<\alpha_{M}.

The companion scale also satisfies τn+1,k≤αM⁢τn,k\tau_{n+1,k}\leq\alpha_{M}\tau_{n,k}.

Fix 0<η<10<\eta<1. Since the order set ℬ\mathcal{B} is finite, (4.10) and (4.11) hold beyond one common threshold. For each sufficiently large primary scale τ=τn,k\tau=\tau_{n,k}, its two rows i=n,n+1i=n,n+1 satisfy

(5.3) 0<Bi,k≤exp⁡((αM+η)⁢τ),|Bi,k⁢x−Ai,k|≤exp⁡(−(1−η)⁢τ).0<B_{i,k}\leq\exp((\alpha_{M}+\eta)\tau),\qquad|B_{i,k}x-A_{i,k}|\leq\exp(-(1-% \eta)\tau).

The companion has a larger scale, which only improves its error. Since τ\tau is a fixed multiple of Δ\Delta for each order in the order set ℬ\mathcal{B}, the o⁢(Δ)o(\Delta) terms are absorbed once MM and η\eta are fixed.

Let qq be any sufficiently large positive integer. Choose the first primary scale for which

(5.4) τ≥log⁡(4⁢q)1−η.\tau\geq\frac{\log(4q)}{1-\eta}.

For sufficiently large qq it has a predecessor beyond the common threshold. The scale-ratio bound therefore gives

(5.5) log⁡(4⁢q)1−η≤τ≤αM⁢log⁡(4⁢q)1−η.\frac{\log(4q)}{1-\eta}\leq\tau\leq\frac{\alpha_{M}\log(4q)}{1-\eta}.

Set

(5.6) β=αM⁢(αM+η)1−η.\beta=\frac{\alpha_{M}(\alpha_{M}+\eta)}{1-\eta}.

For both selected rows, (5.3)–(5.5) imply

(5.7) Bi,k≤(4⁢q)β,q⁢|Bi,k⁢x−Ai,k|≤14.B_{i,k}\leq(4q)^{\beta},\qquad q|B_{i,k}x-A_{i,k}|\leq\frac{1}{4}.

Suppose p∈ℤp\in\mathbb{Z} and

(5.8) |x−pq|<4−(β+1)⁢q−(1+β).\left|x-\frac{p}{q}\right|<4^{-(\beta+1)}q^{-(1+\beta)}.

For i=n,n+1i=n,n+1, the integer Ii,k=Bi,k⁢p−q⁢Ai,kI_{i,k}=B_{i,k}p-qA_{i,k} satisfies

|Ii,k|\displaystyle|I_{i,k}| ≤Bi,k⁢q⁢|pq−x|+q⁢|Bi,k⁢x−Ai,k|\displaystyle\leq B_{i,k}q\left|\frac{p}{q}-x\right|+q|B_{i,k}x-A_{i,k}|
(5.9) <(4⁢q)β⁢q⁢ 4−(β+1)⁢q−(1+β)+14=12.\displaystyle<(4q)^{\beta}q\,4^{-(\beta+1)}q^{-(1+\beta)}+\frac{1}{4}=\frac{1}% {2}.

Both integers would vanish, contrary to (4.13). Hence the reverse of (5.8) holds for every integer pp and every sufficiently large qq, whether or not p/qp/q is reduced or equals a selected approximant.

Let ν>2\nu>2. Since αM→1\alpha_{M}\to 1, choose MM such that 1+αM2<ν1+\alpha_{M}^{2}<\nu, and then choose η>0\eta>0 small enough that 1+β<ν1+\beta<\nu. With these choices fixed, the proved lower bound

|x−pq|≥4−(β+1)⁢q−(1+β)\left|x-\frac{p}{q}\right|\geq 4^{-(\beta+1)}q^{-(1+\beta)}

is larger than q−νq^{-\nu} for all sufficiently large qq. Only finitely many pairs with the remaining denominators can satisfy |x−p/q|<q−ν|x-p/q|<q^{-\nu}. Thus μ⁢(x)≤ν\mu(x)\leq\nu, and letting ν\nu decrease to 22 gives μ⁢(x)≤2\mu(x)\leq 2.

The choices have the order

(5.10) ((λj)j≥0,N)⟶ν>2⟶M,η,ℬ⟶k0,q0⟶(p,q)⟶k,n.\bigl{(}(\lambda_{j})_{j\geq 0},N\bigr{)}\ \longrightarrow\ \nu>2\ % \longrightarrow\ M,\eta,\mathcal{B}\ \longrightarrow\ k_{0},q_{0}\ % \longrightarrow\ (p,q)\ \longrightarrow\ k,n.

The thresholds k0,q0k_{0},q_{0} depend on the sequence and its little-oo modulus.

For the reverse bound, fix an integer R≥1R\geq 1 and partition [0,1)[0,1) into RR intervals of length 1/R1/R. Two fractional parts among {j⁢x}\{jx\}, 0≤j≤R0\leq j\leq R, lie in one interval. Their difference gives integers p,qp,q with

1≤q≤R,|q⁢x−p|<1/R,|x−pq|<1q⁢R≤1q2.1\leq q\leq R,\qquad|qx-p|<1/R,\qquad\left|x-\frac{p}{q}\right|<\frac{1}{qR}% \leq\frac{1}{q^{2}}.

Since xx is irrational, for each fixed DD the finitely many distances ‖q⁢x‖\|qx\|, 1≤q≤D1\leq q\leq D, have a positive minimum mD>0m_{D}>0, where ‖t‖\|t\| denotes distance from tt to the nearest integer. For R>1/mDR>1/m_{D}, the inequality |q⁢x−p|<1/R|qx-p|<1/R forces q>Dq>D. These denominators are unbounded as R→∞R\to\infty, and μ⁢(x)≥2\mu(x)\geq 2.∎

6. Sharpness of the height scale

The little-oo condition cannot be replaced by a bound log⁡H⁢(λj)≤C∗⁢2j\log H(\lambda_{j})\leq C_{*}2^{j} with any constant C∗>0C_{*}>0. Below, small coefficients give exponent greater than 22, and the coefficient 12⁢L\tfrac{1}{2}L gives both a rational and a Liouville sum.

Fix 0<θ<1/30<\theta<1/3, and put

(6.1) mj=⌊θ⁢2j⌋,λj=N(−1)j⁢mj,ej=2j−(−1)j⁢mj.m_{j}=\lfloor\theta 2^{j}\rfloor,\qquad\lambda_{j}=N^{(-1)^{j}m_{j}},\qquad e_% {j}=2^{j}-(-1)^{j}m_{j}.

The weights are positive rationals, with

(6.2) log⁡H⁢(λj)=mj⁢L=θ⁢L⁢2j+O⁢(1).\log H(\lambda_{j})=m_{j}L=\theta L2^{j}+O(1).

The associated sum has the exact digit expansion

x=∑j≥0N−ej.x=\sum_{j\geq 0}N^{-e_{j}}.

The exponents are strictly increasing: for odd jj,

ej+1−ej=2j−mj−mj+1≥(1−3⁢θ)⁢2j>0,e_{j+1}-e_{j}=2^{j}-m_{j}-m_{j+1}\geq(1-3\theta)2^{j}>0,

and for even jj their difference is 2j+mj+mj+1>02^{j}+m_{j}+m_{j+1}>0. The gaps tend to infinity, so the expansion is not eventually periodic and xx is irrational.

Let pj/qjp_{j}/q_{j} be the truncation through index jj, in lowest terms. Its denominator is exactly qj=Nejq_{j}=N^{e_{j}}, because its numerator is 11 modulo NN and hence is coprime to every prime dividing NN. The increasing integer exponents give

(6.3) 0<x−pjqj≤N−ej+11−N−1≤2⁢N−ej+1.0<x-\frac{p_{j}}{q_{j}}\leq\frac{N^{-e_{j+1}}}{1-N^{-1}}\leq 2N^{-e_{j+1}}.

Along even indices,

ej+1ej⟶2⁢(1+θ)1−θ>2.\frac{e_{j+1}}{e_{j}}\longrightarrow\frac{2(1+\theta)}{1-\theta}>2.

For every ν<2⁢(1+θ)/(1−θ)\nu<2(1+\theta)/(1-\theta), (6.3) is less than qj−νq_{j}^{-\nu} at all sufficiently large even indices. Consequently

(6.4) μ⁢(x)≥2⁢(1+θ)1−θ>2.\mu(x)\geq\frac{2(1+\theta)}{1-\theta}>2.

Equivalently, for each 0<κ<L/30<\kappa<L/3 this gives

log⁡H⁢(λj)∼κ⁢2j,μ⁢(x)≥2⁢(L+κ)L−κ.\log H(\lambda_{j})\sim\kappa 2^{j},\qquad\mu(x)\geq\frac{2(L+\kappa)}{L-% \kappa}.

Given any C∗>0C_{*}>0, choose 0<κ<min⁡(C∗,L/3)0<\kappa<\min(C_{*},L/3). Then the same weights satisfy log⁡H⁢(λj)≤C∗⁢2j\log H(\lambda_{j})\leq C_{*}2^{j} for all jj, but their sum has exponent greater than 22.

A rational sum is possible with positive integer weights. Set

(6.5) λ0=N−1,λj=N2j−1−1(j≥1).\lambda_{0}=N-1,\qquad\lambda_{j}=N^{2^{j-1}}-1\quad(j\geq 1).

For j≥1j\geq 1,

λj⁢N−2j=N−2j−1−N−2j,\lambda_{j}N^{-2^{j}}=N^{-2^{j-1}}-N^{-2^{j}},

so the partial sums telescope:

∑j=0mλj⁢N−2j=1−N−2m.\sum_{j=0}^{m}\lambda_{j}N^{-2^{j}}=1-N^{-2^{m}}.

The infinite sum is therefore 11, whereas

(6.6) log⁡H⁢(λj)∼12⁢L⁢ 2j.\log H(\lambda_{j})\sim\frac{1}{2}L\,2^{j}.

The same coefficient also allows a Liouville number. Keep λ0=N−1\lambda_{0}=N-1, and replace the later weights by

λ~j=N2j−1−1+𝟏{j=r2⁢ for some ⁢r≥1}(j≥1).\widetilde{\lambda}_{j}=N^{2^{j-1}}-1+\boldsymbol{1}_{\{j=r^{2}\text{ for some% }r\geq 1\}}\quad(j\geq 1).

These are again positive integers and satisfy (6.6). Their sum is

x~=1+ξN,ξN=∑r≥1N−2r2.\widetilde{x}=1+\xi_{N},\qquad\xi_{N}=\sum_{r\geq 1}N^{-2^{r^{2}}}.

Its digit expansion is not eventually periodic, so ξN\xi_{N} is irrational. The truncation through r=Rr=R has reduced denominator qR=N2R2q_{R}=N^{2^{R^{2}}}, since its numerator is 11 modulo NN, and

0<ξN−∑r=1RN−2r2≤2⁢N−2(R+1)2=2⁢qR−22⁢R+1.0<\xi_{N}-\sum_{r=1}^{R}N^{-2^{r^{2}}}\leq 2N^{-2^{(R+1)^{2}}}=2q_{R}^{-2^{2R+% 1}}.

The same bound holds after adding 11. Since 22⁢R+1→∞2^{2R+1}\to\infty, this proves μ⁢(x~)=∞\mu(\widetilde{x})=\infty.

The height condition is not necessary for an individual series. For example, given an integer b≥2b\geq 2, the weights λj=b−2j\lambda_{j}=b^{-2^{j}} have log⁡H⁢(λj)=(log⁡b)⁢2j\log H(\lambda_{j})=(\log b)2^{j}, but their sum equals ∑j≥0(N⁢b)−2j\sum_{j\geq 0}(Nb)^{-2^{j}}. Theorem 1, applied with base N⁢bNb and constant weights 11, gives exponent 22 for that sum.

Use of AI tools

The author devised the main argument. Codex (OpenAI, GPT-6 Astra) carried out exact checks of the Hankel identities and searched the literature. Claude Code (Anthropic, Claude Opus 5.5) reviewed the arguments and references. The author takes responsibility for the proof and references.

References

  • [1] M. Amou and Y. Bugeaud, Exponents of Diophantine approximation and expansions in integer bases, J. Lond. Math. Soc. (2) 81 (2010), 297–316.
  • [2] Y. Bugeaud, G.-N. Han, Z.-Y. Wen, and J.-Y. Yao, Hankel determinants, Padé approximations, and irrationality exponents, Int. Math. Res. Not. IMRN 2016 (2016), no. 5, 1467–1496, https://doi.org/10.1093/imrn/rnv185.
  • [3] D. Duverney, Irrationality of fast converging series of rational numbers, J. Math. Sci. Univ. Tokyo 8 (2001), 275–316.
  • [4] D. Duverney, Irrationality of certain fast converging series and infinite products, Hokkaido Math. J. 53 (2024), no. 2, 377–394, https://doi.org/10.14492/hokmj/2022-679.
  • [5] D. Duverney, T. Kurosawa, and I. Shiokawa, Irrationality exponents of certain fast converging series of rational numbers, Tsukuba J. Math. 44 (2020), no. 2, 235–250, https://doi.org/10.21099/tkbjm/20204402235.
  • [6] K. Nishioka, New approach in Mahler’s method, J. Reine Angew. Math. 407 (1990), 202–219.
  • [7] A. Rajchert, On the irrationality exponents of Mahler numbers, arXiv:2411.10733 (2024).
  • [8] J. O. Shallit, Simple continued fractions for some irrational numbers, J. Number Theory 11 (1979), no. 2, 209–217, doi:10.1016/0022-314X(79)90040-4.
  • [9] L.-H. Su, Binary-valuation identities and lacunary continued fractions in integer sequences, Zenodo record 23676031 (2026), https://doi.org/10.5281/zenodo.23676031.