Contents

Irrationality of the dilogarithm at 1/4

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

We prove that Li2⁡(1/4)\operatorname{Li}_{2}(1/4) is irrational. Irrationality of Li2⁡(1/s)\operatorname{Li}_{2}(1/s) was known for integers s≤−5s\leq-5 and s≥6s\geq 6 by work of Hata and of Rhin and Viola, and Prellberg recently proved it for s=−4,5,−3s=-4,5,-3. The linear forms in 11 and Li2⁡(1/4)\operatorname{Li}_{2}(1/4) come from one double integral of Viola and Zudilin at z=4z=4. We expand it into Rhin–Viola integrals in three ways and apply their factorial transformations to each term. This gives a common factor of the coefficients of the NNth form. The third expansion adds the primes between 265⁢N265N and 322⁢N322N to this factor, which is too small without them. We bound the integral by the weighted arithmetic-geometric mean inequality and by concavity on circular arcs.

Key words and phrases:
dilogarithm, irrationality, permutation group method
2020 Mathematics Subject Classification:
Primary 11J72; Secondary 33B30

1. Introduction

For |w|≤1|w|\leq 1 let Li2⁡(w)=∑n≥1wn/n2\operatorname{Li}_{2}(w)=\sum_{n\geq 1}w^{n}/n^{2}. Hata [3] proved that Li2⁡(1/s)\operatorname{Li}_{2}(1/s) is irrational for every integer s≤−5s\leq-5 and every s≥7s\geq 7. Rhin and Viola adapted their permutation group method [5] to the dilogarithm and settled s=6s=6 [6]. They later treated negative arguments [7]. Viola and Zudilin [8] introduced a six-parameter family of double integrals. In 2024 Calegari, Dimitrov and Tang [1, Remark 2.8.2 and Section 15.2] listed the integers still open: s∈{−4,−3,−2,2,3,4,5}s\in\{-4,-3,-2,2,3,4,5\}. Prellberg’s 2026 preprint [4] treats s=−4,5,−3s=-4,5,-3. We prove the case s=4s=4.

Theorem 1.

The number Li2⁡(1/4)\operatorname{Li}_{2}(1/4) is irrational.

By Landen’s identity [2, (25.12.3)], Li2⁡(1/4)+Li2⁡(−1/3)=−12⁢log2⁡(3/4)\operatorname{Li}_{2}(1/4)+\operatorname{Li}_{2}(-1/3)=-\frac{1}{2}\log^{2}(3/4), so Theorem 1 does not follow directly from the case s=−3s=-3.

Put θ=Li2⁡(1/4)\theta=\operatorname{Li}_{2}(1/4), dm=lcm⁡(1,…,m)d_{m}=\operatorname{lcm}(1,\dots,m), d0=1d_{0}=1, and for N≥1N\geq 1

(1.1) GN\displaystyle G_{N} =J4⁢(240⁢N,240⁢N,190⁢N,157⁢N,215⁢N,165⁢N),\displaystyle=J_{4}(240N,240N,190N,157N,215N,165N),
DN\displaystyle D_{N} =d323⁢N⁢d322⁢N⁢ 4132⁢N⁢ 3107⁢N,\displaystyle=d_{323N}\,d_{322N}\,4^{132N}\,3^{107N},

with J4J_{4} as in Section 2. By [8, Lemma 2.1], DN⁢GN∈ℤ+ℤ⁢θD_{N}G_{N}\in\mathbb{Z}+\mathbb{Z}\theta. Sections 3 and 4 give ΔN∣DN\Delta_{N}\mid D_{N} with

(DN/ΔN)⁢GN∈ℤ+ℤ⁢θ,\displaystyle(D_{N}/\Delta_{N})\,G_{N}\in\mathbb{Z}+\mathbb{Z}\theta,
limN→∞log⁡ΔN40⁢N=δ>4.7670,limN→∞log⁡DN40⁢N<23.63856,\displaystyle\lim_{N\to\infty}\frac{\log\Delta_{N}}{40N}=\delta>4.7670,\qquad% \lim_{N\to\infty}\frac{\log D_{N}}{40N}<23.63856,

and Sections 5 and 6 give

GN>0⁢for large ⁢N,lim supN→∞log⁡GN40⁢N≤−18.87333.G_{N}>0\ \text{for large }N,\qquad\limsup_{N\to\infty}\frac{\log G_{N}}{40N}% \leq-18.87333.

Since 23.63856−4.7670−18.87333<023.63856-4.7670-18.87333<0, Theorem 1 follows.

The arithmetic follows [4, Section 3.2]. Identity (2.1) for GNG_{N} and for its image under (F2) gives the analogues of [4, (3.11)–(3.12)]. The factorial transformations of [6] act on each term. For 265⁢N<p<322⁢N265N<p<322N these expansions give only M=0M=0 in Lemma 3.2. These primes account for 57/4057/40 of δ\delta, and the rest of δ\delta is below 3.35<23.63856−18.873333.35<23.63856-18.87333. Expansion (2.2) gives one power of each such pp. The bounds of Lemma 3.2 depend only on N/pN/p, so we need not exclude the exceptional primes of [4, (3.6)–(3.7)]. One linear form suffices, since GN>0G_{N}>0 for large NN.

Two Python scripts recheck only part of the proof (Appendix C). The proof is complete without them. The use of AI tools is described at the end of the paper.

2. Integrals and known results

Let z>1z>1. For integers h,j,k,l,m,q≥0h,j,k,l,m,q\geq 0 with j+k−m,j+q−m,h+m−k,h+q−k≥0j+k-m,\ j+q-m,\ h+m-k,\ h+q-k\geq 0 put

Rz⁢(x,y)=zk−l−q⁢xj⁢(1−x)h⁢yk⁢(1−y)l⁢(1−y+z⁢y)j+q−m(x⁢(1−y)+z⁢y)j+k−m+1,R_{z}(x,y)=z^{k-l-q}\,\frac{x^{j}(1-x)^{h}\,y^{k}(1-y)^{l}\,(1-y+zy)^{j+q-m}}{% \bigl{(}x(1-y)+zy\bigr{)}^{j+k-m+1}},

and, with small positively oriented circles,

Jz(0)\displaystyle J_{z}^{(0)} =∫01∫01Rz⁢𝑑y⁢𝑑x,\displaystyle=\int_{0}^{1}\!\!\int_{0}^{1}R_{z}\,dy\,dx, Jz(1)\displaystyle J_{z}^{(1)} =∫0112⁢π⁢i⁢∮|y−xx−z|=εRz⁢𝑑y⁢𝑑x,\displaystyle=\int_{0}^{1}\frac{1}{2\pi i}\oint_{|y-\frac{x}{x-z}|=\varepsilon% }R_{z}\,dy\,dx,
Jz(2)\displaystyle J_{z}^{(2)} =12⁢π⁢i⁢∮|x−z|=ε′12⁢π⁢i⁢∮|y−xx−z|=εRz⁢𝑑y⁢𝑑x,\displaystyle=\frac{1}{2\pi i}\oint_{|x-z|=\varepsilon^{\prime}}\frac{1}{2\pi i% }\oint_{|y-\frac{x}{x-z}|=\varepsilon}R_{z}\,dy\,dx, Jz\displaystyle J_{z} =Jz(0)−(log⁡z)⁢Jz(1).\displaystyle=J_{z}^{(0)}-(\log z)J_{z}^{(1)}.

For t=(h,j,k,l,m)∈ℤ≥05t=(h,j,k,l,m)\in\mathbb{Z}_{\geq 0}^{5} define Iz(0)⁢(t)I_{z}^{(0)}(t), Iz(1)⁢(t)I_{z}^{(1)}(t), Iz(2)⁢(t)I_{z}^{(2)}(t) and Iz⁢(t)I_{z}(t) in the same way from

z−l−m⁢xj⁢(1−x)h⁢yk⁢(1−y)l(x⁢(1−y)+z⁢y)j+k−m+1[6, (2.1)–(2.4)].z^{-l-m}\,\frac{x^{j}(1-x)^{h}\,y^{k}(1-y)^{l}}{\bigl{(}x(1-y)+zy\bigr{)}^{j+k% -m+1}}\qquad\text{\cite[cite]{[\@@bibref{}{RV05}{}{}, (2.1)--(2.4)]}}.

For 𝒥=Jz\mathcal{J}=J_{z} or 𝒥=Iz⁢(t)\mathcal{J}=I_{z}(t), with components 𝒥(0),𝒥(1),𝒥(2)\mathcal{J}^{(0)},\mathcal{J}^{(1)},\mathcal{J}^{(2)}, put

c⁢(𝒥)=(c1⁢(𝒥),c2⁢(𝒥))=(𝒥+Li2⁡(1/z)⁢𝒥(2),𝒥(2)).c(\mathcal{J})=\bigl{(}c_{1}(\mathcal{J}),c_{2}(\mathcal{J})\bigr{)}=\bigl{(}% \mathcal{J}+\operatorname{Li}_{2}(1/z)\,\mathcal{J}^{(2)},\ \mathcal{J}^{(2)}% \bigr{)}.

For t=(h,j,k,l,m)t=(h,j,k,l,m) let

u⁢(t)=(l+m−j,h+m−k,h+j−l,j+k−m),T⁢(t)=h!⁢j!⁢k!⁢l!⁢m!,\displaystyle u(t)=(l+m-j,\ h+m-k,\ h+j-l,\ j+k-m),\qquad T(t)=h!\,j!\,k!\,l!% \,m!,
H⁢(t)=maxi⁡ui,K⁢(t)=max⁡{u1,min⁡(u2,u3),u4},\displaystyle H(t)=\max_{i}u_{i},\qquad K(t)=\max\{u_{1},\min(u_{2},u_{3}),u_{% 4}\},

and call tt admissible if u⁢(t)∈ℤ≥04u(t)\in\mathbb{Z}_{\geq 0}^{4}. Put

ρ⁢(t)=(h,m,l,k,j),σ⁢(t)=(h+m−k,j+k−m,m,l,k),\rho(t)=(h,m,l,k,j),\qquad\sigma(t)=(h+m-k,\ j+k-m,\ m,\ l,\ k),

and let O⁢(t)O(t) be the orbit of tt under the group generated by ρ\rho and σ\sigma. Both maps permute the multiset {h,j,k,l,m,u1,u2,u3,u4}\{h,j,k,l,m,u_{1},u_{2},u_{3},u_{4}\} [6, (3.2), (3.15)], so every s∈O⁢(t)s\in O(t) is admissible when tt is.

  1. (F1)

    [8, Lemma 2.1] Let H1=max⁡{l+q,h+m−k,h+j−l,j+k−m}H_{1}=\max\{l+q,\,h+m-k,\,h+j-l,\,j+k-m\}, H2=max⁡{l+q,min⁡(h+m−k,h+j−l),j+k−m}H_{2}=\max\{l+q,\,\min(h+m-k,h+j-l),\,j+k-m\}, α=max⁡{0,l+q−k,l+q−m}\alpha=\max\{0,l+q-k,l+q-m\} and β=max⁡{0,k+l−h}\beta=\max\{0,k+l-h\}. There are P,Q∈ℤ⁢[z]P,Q\in\mathbb{Z}[z] with

    dH1⁢dH2⁢zα⁢(1−z)β⁢c⁢(Jz)=(P⁢(z),Q⁢(z)).d_{H_{1}}d_{H_{2}}\,z^{\alpha}(1-z)^{\beta}\,c(J_{z})=(P(z),Q(z)).
  2. (F2)

    [8, Lemma 3.1] c⁢(Jz⁢(h,j,k,l,m,q))=c⁢(Jz⁢(j,h,m,l,k,q))c(J_{z}(h,j,k,l,m,q))=c(J_{z}(j,h,m,l,k,q)).

  3. (F3)

    [6, Theorem 2.1 and (2.9)] Let α⁢(t)=max⁡{j+k,k+l,l+m}\alpha(t)=\max\{j+k,k+l,l+m\} and β⁢(t)=max⁡{0,k+l−h}\beta(t)=\max\{0,k+l-h\}. There are Pt,Qt∈ℤ⁢[z]P_{t},Q_{t}\in\mathbb{Z}[z] with

    dH⁢(t)⁢dK⁢(t)⁢zα⁢(t)⁢(z−1)β⁢(t)⁢c⁢(Iz⁢(t))=(Pt⁢(z),Qt⁢(z)).d_{H(t)}d_{K(t)}\,z^{\alpha(t)}(z-1)^{\beta(t)}\,c(I_{z}(t))=(P_{t}(z),Q_{t}(z% )).
  4. (F4)

    [6, (3.10)–(3.16)] If tt is admissible and s∈O⁢(t)s\in O(t), then c⁢(Iz⁢(t))/T⁢(t)=c⁢(Iz⁢(s))/T⁢(s)c(I_{z}(t))/T(t)=c(I_{z}(s))/T(s).

In the sources, (F1) and (F3) read φ⁢𝒥=P−Q⁢Li2⁡(1/z)\varphi\mathcal{J}=P-Q\operatorname{Li}_{2}(1/z) and φ⁢𝒥(2)=Q\varphi\mathcal{J}^{(2)}=Q, with φ\varphi the displayed multiplier; (F2) and (F4) are stated there for each component. Numbering in [8] refers to the preprint version.

Lemma 2.1.

Let a=j+q−ma=j+q-m. Then

(2.1) c⁢(Jz⁢(h,j,k,l,m,q))\displaystyle c(J_{z}(h,j,k,l,m,q)) =∑λ=0a(aλ)⁢zj+k+λ⁢c⁢(Iz⁢(h,j,k+λ,l+a−λ,m+λ)),\displaystyle=\sum_{\lambda=0}^{a}\binom{a}{\lambda}z^{j+k+\lambda}\,c(I_{z}(h% ,\,j,\,k+\lambda,\,l+a-\lambda,\,m+\lambda)),
(2.2) c⁢(Jz⁢(h,j,k,l,m,q))\displaystyle c(J_{z}(h,j,k,l,m,q)) =∑λ=0a(aλ)⁢zj+k⁢(1−z)λ⁢c⁢(Iz⁢(h,j,k,l+λ,m)).\displaystyle=\sum_{\lambda=0}^{a}\binom{a}{\lambda}z^{j+k}(1-z)^{\lambda}\,c(% I_{z}(h,\,j,\,k,\,l+\lambda,\,m)).
Proof.

Expand (1−y+z⁢y)a(1-y+zy)^{a} as ((1−y)+z⁢y)a((1-y)+zy)^{a} and as (z+(1−z)⁢(1−y))a(z+(1-z)(1-y))^{a}. Each term has the denominator and the pole y=x/(x−z)y=x/(x-z) of the corresponding IzI_{z}-integrand. The powers of zz are zk−l−q+λ⋅z(l+a−λ)+(m+λ)=zj+k+λz^{k-l-q+\lambda}\cdot z^{(l+a-\lambda)+(m+\lambda)}=z^{j+k+\lambda} and zk−l−q+a−λ⋅z(l+λ)+m=zj+kz^{k-l-q+a-\lambda}\cdot z^{(l+\lambda)+m}=z^{j+k}. The identities hold for each component, hence for cc. ∎

Identity (2.1) is used in the proof of [8, Lemma 2.1] and in [4, (3.11)–(3.12)].

3. The divisor

3.1. Local bounds

For the tuple in (1.1), (F1) gives H1=323⁢NH_{1}=323N, H2=322⁢NH_{2}=322N, α=132⁢N\alpha=132N, β=107⁢N\beta=107N. Since (1−z)β=±3107⁢N(1-z)^{\beta}=\pm 3^{107N} at z=4z=4,

(3.1) DN⁢c⁢(GN)∈ℤ2,GN=c1⁢(GN)−θ⁢c2⁢(GN).D_{N}\,c(G_{N})\in\mathbb{Z}^{2},\qquad G_{N}=c_{1}(G_{N})-\theta\,c_{2}(G_{N}).

Fix N≥1N\geq 1 and a prime p>3p>3 with p2>430⁢Np^{2}>430N. Put x=N/px=N/p and Fa=⌊a⁢x⌋F_{a}=\lfloor ax\rfloor, and let [⋅][\,\cdot\,] be the Iverson bracket. For 0≤n≤430⁢N0\leq n\leq 430N, vp⁢(n!)=⌊n/p⌋v_{p}(n!)=\lfloor n/p\rfloor and vp⁢(dn)=[n≥p]v_{p}(d_{n})=[\,n\geq p\,].

Lemma 3.1.

Let tt be admissible with all entries of tt and u⁢(t)u(t) in [0,430⁢N][0,430N], and let s∈O⁢(t)s\in O(t). Then, for i=1,2i=1,2,

vp⁢(ci⁢(I4⁢(t)))≥∑ν=15(⌊tνp⌋−⌊sνp⌋)−[H⁢(s)≥p]−[K⁢(s)≥p].v_{p}\bigl{(}c_{i}(I_{4}(t))\bigr{)}\ \geq\ \sum_{\nu=1}^{5}\Bigl{(}\lfloor% \frac{t_{\nu}}{p}\rfloor-\lfloor\frac{s_{\nu}}{p}\rfloor\Bigr{)}-[\,H(s)\geq p% \,]-[\,K(s)\geq p\,].
Proof.

By (F4), c⁢(I4⁢(t))=T⁢(t)⁢T⁢(s)−1⁢c⁢(I4⁢(s))c(I_{4}(t))=T(t)T(s)^{-1}c(I_{4}(s)). The entries of ss and u⁢(s)u(s) are those of tt and u⁢(t)u(t) in some order. Apply (F3) to ss, where z=4z=4 and z−1=3z-1=3 are units at pp. ∎

Lemma 3.2.

Suppose p<322⁢Np<322N. For b∈{190,215}b\in\{190,215\} put eb=2⁢b−165e_{b}=2b-165 and

C\displaystyle C =2⁢F240−F265−F215,\displaystyle=2F_{240}-F_{265}-F_{215},
Ub\displaystyle U_{b} =2⁢F240+2⁢Fb−Feb−F323−F322,\displaystyle=2F_{240}+2F_{b}-F_{e_{b}}-F_{323}-F_{322},
Vb\displaystyle V_{b} =2⁢Fb+F157−Feb−F322.\displaystyle=2F_{b}+F_{157}-F_{e_{b}}-F_{322}.

Then, for i=1,2i=1,2,

(3.2) vp⁢(DN⁢ci⁢(GN))≥M:=max⁡{0,C,U190,U215,V190,V215}.v_{p}\bigl{(}D_{N}\,c_{i}(G_{N})\bigr{)}\ \geq\ M:=\max\{0,\,C,\,U_{190},\,U_{% 215},\,V_{190},\,V_{215}\}.

If moreover p>265⁢Np>265N, then vp⁢(DN⁢ci⁢(GN))≥1v_{p}(D_{N}\,c_{i}(G_{N}))\geq 1.

Proof.

Here vp⁢(DN)=2v_{p}(D_{N})=2. By (F2), c⁢(GN)c(G_{N}) is unchanged if (1.1) is replaced by (240⁢N,240⁢N,215⁢N,157⁢N,190⁢N,165⁢N)(240N,240N,215N,157N,190N,165N). So (2.1), applied to (1.1) for b=190b=190 and to this tuple for b=215b=215, gives

c⁢(GN)=∑λ=0b⁢N(b⁢Nλ)⁢4(240+b)⁢N+λ⁢c⁢(I4⁢(t)),c(G_{N})=\sum_{\lambda=0}^{bN}\binom{bN}{\lambda}4^{(240+b)N+\lambda}\,c(I_{4}% (t)),

where t=(240,240,b,157+b,405−b)⁢N+(0,0,1,−1,1)⁢λt=(240,240,b,157+b,405-b)N+(0,0,1,-1,1)\lambda. Here u⁢(t)=(322, 645−2⁢b, 323−b,eb)⁢N+(0,0,1,0)⁢λu(t)=(322,\,645-2b,\,323-b,\,e_{b})N+(0,0,1,0)\lambda; all entries of tt and u⁢(t)u(t) lie in [0,430⁢N][0,430N]. The tuples

s1=σ⁢t\displaystyle s_{1}=\sigma t =(645−2⁢b,eb, 405−b, 157+b,b)⁢N+(0,0,1,−1,1)⁢λ,\displaystyle=(645-2b,\ e_{b},\ 405-b,\ 157+b,\ b)N+(0,0,1,-1,1)\lambda,
s2=σ⁢ρ⁢σ⁢t\displaystyle s_{2}=\sigma\rho\sigma t =(323−b, 322,eb, 405−b, 157+b)⁢N+(1,0,0,1,−1)⁢λ,\displaystyle=(323-b,\ 322,\ e_{b},\ 405-b,\ 157+b)N+(1,0,0,1,-1)\lambda,
s3=σ⁢ρ⁢σ⁢ρ⁢σ⁢t\displaystyle s_{3}=\sigma\rho\sigma\rho\sigma t =(240, 240, 322,eb, 405−b)⁢N+(0,0,0,0,1)⁢λ\displaystyle=(240,\ 240,\ 322,\ e_{b},\ 405-b)N+(0,0,0,0,1)\lambda

lie in O⁢(t)O(t). Put τ=λ/p\tau=\lambda/p. Then vp⁢(b⁢Nλ)=Fb−⌊τ⌋−⌊b⁢x−τ⌋v_{p}\binom{bN}{\lambda}=F_{b}-\lfloor\tau\rfloor-\lfloor bx-\tau\rfloor. Also [H⁢(s)≥p]+[K⁢(s)≥p]≤2=vp⁢(DN)[\,H(s)\geq p\,]+[\,K(s)\geq p\,]\leq 2=v_{p}(D_{N}) for each s∈O⁢(t)s\in O(t), so Lemma 3.1 shows that the λ\lambda-th term of DN⁢ci⁢(GN)D_{N}c_{i}(G_{N}) has valuation at least

g⁢(s)=∑ν(⌊tν/p⌋−⌊sν/p⌋)+Fb−⌊τ⌋−⌊b⁢x−τ⌋.g(s)=\sum_{\nu}\bigl{(}\lfloor t_{\nu}/p\rfloor-\lfloor s_{\nu}/p\rfloor\bigr{% )}+F_{b}-\lfloor\tau\rfloor-\lfloor bx-\tau\rfloor.

Direct subtraction gives

g⁢(s1)\displaystyle g(s_{1}) =C+(Fb−⌊τ⌋−⌊b⁢x−τ⌋),\displaystyle=C+\bigl{(}F_{b}-\lfloor\tau\rfloor-\lfloor bx-\tau\rfloor\bigr{)},
g⁢(s2)\displaystyle g(s_{2}) =2⁢F240+Fb−Feb−F322+(⌊b⁢x+τ⌋−⌊τ⌋)\displaystyle=2F_{240}+F_{b}-F_{e_{b}}-F_{322}+\bigl{(}\lfloor bx+\tau\rfloor-% \lfloor\tau\rfloor\bigr{)}
−(⌊b⁢x−τ⌋+⌊(323−b)⁢x+τ⌋),\displaystyle\qquad-\bigl{(}\lfloor bx-\tau\rfloor+\lfloor(323-b)x+\tau\rfloor% \bigr{)},
g⁢(s3)\displaystyle g(s_{3}) =Fb−Feb−F322+(⌊b⁢x+τ⌋−⌊τ⌋)\displaystyle=F_{b}-F_{e_{b}}-F_{322}+\bigl{(}\lfloor bx+\tau\rfloor-\lfloor% \tau\rfloor\bigr{)}
+(⌊(157+b)⁢x−τ⌋−⌊b⁢x−τ⌋).\displaystyle\qquad+\bigl{(}\lfloor(157+b)x-\tau\rfloor-\lfloor bx-\tau\rfloor% \bigr{)}.

By ⌊y⌋+⌊w⌋≤⌊y+w⌋\lfloor y\rfloor+\lfloor w\rfloor\leq\lfloor y+w\rfloor,

Fb−⌊τ⌋−⌊b⁢x−τ⌋≥0,⌊b⁢x+τ⌋−⌊τ⌋≥Fb,\displaystyle F_{b}-\lfloor\tau\rfloor-\lfloor bx-\tau\rfloor\geq 0,\qquad% \lfloor bx+\tau\rfloor-\lfloor\tau\rfloor\geq F_{b},
⌊(157+b)⁢x−τ⌋−⌊b⁢x−τ⌋≥F157,⌊b⁢x−τ⌋+⌊(323−b)⁢x+τ⌋≤F323.\displaystyle\lfloor(157+b)x-\tau\rfloor-\lfloor bx-\tau\rfloor\geq F_{157},% \qquad\lfloor bx-\tau\rfloor+\lfloor(323-b)x+\tau\rfloor\leq F_{323}.

Hence g⁢(s1)≥Cg(s_{1})\geq C, g⁢(s2)≥Ubg(s_{2})\geq U_{b} and g⁢(s3)≥Vbg(s_{3})\geq V_{b} for every λ\lambda. The ultrametric inequality and (3.1) give (3.2).

Now let p>265⁢Np>265N. By (2.2),

c⁢(GN)=∑λ=0190⁢N(190⁢Nλ)⁢4430⁢N⁢(−3)λ⁢c⁢(I4⁢(t′)),c(G_{N})=\sum_{\lambda=0}^{190N}\binom{190N}{\lambda}4^{430N}(-3)^{\lambda}\,c% (I_{4}(t^{\prime})),

where

t′\displaystyle t^{\prime} =(240,240,190,157,215)⁢N+(0,0,0,1,0)⁢λ,\displaystyle=(240,240,190,157,215)N+(0,0,0,1,0)\lambda,
u⁢(t′)\displaystyle u(t^{\prime}) =(132,265,323,215)⁢N+(1,0,−1,0)⁢λ,\displaystyle=(132,265,323,215)N+(1,0,-1,0)\lambda,
s′=σ⁢ρ⁢σ⁢t′\displaystyle s^{\prime}=\sigma\rho\sigma t^{\prime} =(323,132,215,215,157)⁢N+(−1,1,0,0,1)⁢λ,\displaystyle=(323,132,215,215,157)N+(-1,1,0,0,1)\lambda,
u⁢(s′)\displaystyle u(s^{\prime}) =(240,265,240,190)⁢N.\displaystyle=(240,265,240,190)N.

So [H⁢(s′)≥p]=[K⁢(s′)≥p]=0[\,H(s^{\prime})\geq p\,]=[\,K(s^{\prime})\geq p\,]=0. Also vp⁢(190⁢Nλ)=0v_{p}\binom{190N}{\lambda}=0 and F240=F215=F190=0F_{240}=F_{215}=F_{190}=0. By Lemma 3.1 and vp⁢(DN)=2v_{p}(D_{N})=2, each term of DN⁢ci⁢(GN)D_{N}c_{i}(G_{N}) has valuation at least 2−⌊323⁢x−τ⌋−⌊132⁢x+τ⌋≥2−⌊455⁢x⌋≥12-\lfloor 323x-\tau\rfloor-\lfloor 132x+\tau\rfloor\geq 2-\lfloor 455x\rfloor\geq 1, as 455⁢x<2455x<2. ∎

3.2. Periodic intervals

Since 55 divides 240240, 265265 and 215215, and 2⋅240=265+2152\cdot 240=265+215, we get C⁢(x+1/5)=C⁢(x)C(x+1/5)=C(x). For 1≤k≤471\leq k\leq 47 put jk=⌊5⁢k/48⌋j_{k}=\lfloor 5k/48\rfloor, ϱk=5⁢k−48⁢jk\varrho_{k}=5k-48j_{k}, ak=k/240a_{k}=k/240 and

bk={(k−jk)/215,ϱk≤21,(k+jk+1)/265,ϱk≥22.b_{k}=\begin{cases}(k-j_{k})/215,&\varrho_{k}\leq 21,\\ (k+j_{k}+1)/265,&\varrho_{k}\geq 22.\end{cases}
Lemma 3.3.

For 1≤k≤471\leq k\leq 47 one has ak<bk≤(k+1)/240a_{k}<b_{k}\leq(k+1)/240 and C=1C=1 on (ak,bk)(a_{k},b_{k}).

Proof.

Here 0<ϱk<480<\varrho_{k}<48, (k−jk)/215−ak=ϱk/10320(k-j_{k})/215-a_{k}=\varrho_{k}/10320, (k+jk+1)/265−ak=(48−ϱk)/12720(k+j_{k}+1)/265-a_{k}=(48-\varrho_{k})/12720 and 265⁢(k−jk)−215⁢(k+jk+1)=10⁢ϱk−215265(k-j_{k})-215(k+j_{k}+1)=10\varrho_{k}-215. So bk=min⁡{(k−jk)/215,(k+jk+1)/265}>akb_{k}=\min\{(k-j_{k})/215,\,(k+j_{k}+1)/265\}>a_{k}, and 48⁢jk≤5⁢k48j_{k}\leq 5k gives bk≤(k+jk+1)/265≤(k+1)/240b_{k}\leq(k+j_{k}+1)/265\leq(k+1)/240. For ak<x<bka_{k}<x<b_{k},

k−jk−1<k−5⁢k48<215⁢x<k−jk,k+jk≤k+5⁢k48<265⁢x<k+jk+1,k-j_{k}-1<k-\tfrac{5k}{48}<215x<k-j_{k},\qquad k+j_{k}\leq k+\tfrac{5k}{48}<26% 5x<k+j_{k}+1,

and F240=kF_{240}=k. Hence C=2⁢k−(k−jk−1)−(k+jk)=1C=2k-(k-j_{k}-1)-(k+j_{k})=1. ∎

Put 𝒞=⋃r=09⋃k=147(r/5+ak,r/5+bk)⊂(1/240,2)\mathcal{C}=\bigcup_{r=0}^{9}\bigcup_{k=1}^{47}\,(r/5+a_{k},\ r/5+b_{k})% \subset(1/240,2); by Lemma 3.3 these 470470 intervals are pairwise disjoint. Let ℰ1,…,ℰ18\mathcal{E}_{1},\dots,\mathcal{E}_{18} be the open intervals

(1/322, 1/265)(1/215, 2/323)(2/215, 3/322)(3/215, 4/265),(4/190, 7/323)(7/265, 9/322)(5/157, 11/323)(7/190, 12/322),(9/215, 14/323)(11/215, 17/322)(11/190, 19/323)(17/265, 21/322),(11/157, 23/323)(14/190, 24/322)(15/190, 26/323)(19/215, 29/322),(21/190, 36/322)(22/190, 38/323).\begin{array}[]{llll}(1/322,\,1/265)&(1/215,\,2/323)&(2/215,\,3/322)&(3/215,\,% 4/265),\\ (4/190,\,7/323)&(7/265,\,9/322)&(5/157,\,11/323)&(7/190,\,12/322),\\ (9/215,\,14/323)&(11/215,\,17/322)&(11/190,\,19/323)&(17/265,\,21/322),\\ (11/157,\,23/323)&(14/190,\,24/322)&(15/190,\,26/323)&(19/215,\,29/322),\\ (21/190,\,36/322)&(22/190,\,38/323).\end{array}

They are pairwise disjoint and lie in (1/322,1/5)(1/322,1/5). Define

μ⁢(x)=𝟏𝒞⁢(x)+∑i=118𝟏ℰi⁢(x).\mu(x)=\mathbf{1}_{\mathcal{C}}(x)+\sum_{i=1}^{18}\mathbf{1}_{\mathcal{E}_{i}}% (x).
Proposition 3.4.

Let N≥1N\geq 1 and let p>3p>3 be a prime with p2>430⁢Np^{2}>430N. Then μ⁢(N/p)≤vp⁢(DN)\mu(N/p)\leq v_{p}(D_{N}) and vp⁢(DN⁢ci⁢(GN))≥μ⁢(N/p)v_{p}(D_{N}\,c_{i}(G_{N}))\geq\mu(N/p) for i=1,2i=1,2.

Proof.

Let x=N/px=N/p with μ⁢(x)>0\mu(x)>0. Then 1/322<x<21/322<x<2, so p<322⁢Np<322N, vp⁢(DN)=2v_{p}(D_{N})=2 and μ⁢(x)≤2\mu(x)\leq 2. If x∉⋃iℰix\notin\bigcup_{i}\mathcal{E}_{i}, then μ⁢(x)=𝟏𝒞⁢(x)≤[C=1]≤M\mu(x)=\mathbf{1}_{\mathcal{C}}(x)\leq[\,C=1\,]\leq M by Lemmas 3.3 and 3.2. If x∈ℰ1x\in\mathcal{E}_{1}, then x∉𝒞x\notin\mathcal{C} and p>265⁢Np>265N, so Lemma 3.2 gives vp⁢(DN⁢ci⁢(GN))≥1=μ⁢(x)v_{p}(D_{N}\,c_{i}(G_{N}))\geq 1=\mu(x). If x∈ℰ2∪⋯∪ℰ18x\in\mathcal{E}_{2}\cup\dots\cup\mathcal{E}_{18}, then M≥1+[C=1]≥μ⁢(x)M\geq 1+[\,C=1\,]\geq\mu(x) by Table A.1, which lists the floors FaF_{a} for a∈{157,190,215,240,265,322,323}a\in\{157,190,215,240,265,322,323\} on pieces with no jump inside. ∎

4. Density

Lemma 4.1.

Let ΔN=∏pμ⁢(N/p)\Delta_{N}=\prod p^{\mu(N/p)} over primes p>3p>3 with p2>430⁢Np^{2}>430N. Then ΔN∣DN\Delta_{N}\mid D_{N}, (DN/ΔN)⁢c⁢(GN)∈ℤ2(D_{N}/\Delta_{N})\,c(G_{N})\in\mathbb{Z}^{2}, and

limN→∞log⁡ΔN40⁢N\displaystyle\lim_{N\to\infty}\frac{\log\Delta_{N}}{40N} =δ:=140⁢∫02μ⁢(x)⁢d⁢xx2>4.7670,\displaystyle=\delta:=\frac{1}{40}\int_{0}^{2}\mu(x)\,\frac{dx}{x^{2}}>4.7670,
limN→∞log⁡DN40⁢N\displaystyle\lim_{N\to\infty}\frac{\log D_{N}}{40N} =cD:=645+132⁢log⁡4+107⁢log⁡340<23.63856.\displaystyle=c_{D}:=\frac{645+132\log 4+107\log 3}{40}<23.63856.
Proof.

The first two claims follow from Proposition 3.4 and (3.1). If μ⁢(N/p)>0\mu(N/p)>0, then p>N/2p>N/2, so p>3p>3 and p2>430⁢Np^{2}>430N for N>1720N>1720. For each of the 488488 intervals II of 𝒞\mathcal{C} and ℰ1,…,ℰ18\mathcal{E}_{1},\dots,\mathcal{E}_{18}, the prime number theorem gives

∑N/p∈Ilog⁡p=N⁢∫Ix−2⁢𝑑x+o⁢(N).\sum_{N/p\in I}\log p=N\int_{I}x^{-2}\,dx+o(N).

Summing over II gives δ\delta. Likewise log⁡dn=n+o⁢(n)\log d_{n}=n+o(n) gives cDc_{D}, and cD<23.63856c_{D}<23.63856 by Table B.1.

The intervals of 𝒞\mathcal{C} with r=0r=0 contribute

δ0=140⁢∑k=147(1ak−1bk)=140⁢(∑k=147240k−∑ϱk≤21215k−jk−∑ϱk≥22265k+jk+1)>1.6187,\delta_{0}=\frac{1}{40}\sum_{k=1}^{47}\Bigl{(}\frac{1}{a_{k}}-\frac{1}{b_{k}}% \Bigr{)}=\frac{1}{40}\Bigl{(}\sum_{k=1}^{47}\frac{240}{k}-\sum_{\varrho_{k}% \leq 21}\frac{215}{k-j_{k}}-\sum_{\varrho_{k}\geq 22}\frac{265}{k+j_{k}+1}% \Bigr{)}>1.6187,

with the two cases listed in Table A.2. Let ℓ=∑k(bk−ak)=1139/22790\ell=\sum_{k}(b_{k}-a_{k})=1139/22790 and y¯=ℓ−1⁢∑k∫akbky⁢𝑑y=164041/1640160\bar{y}=\ell^{-1}\sum_{k}\int_{a_{k}}^{b_{k}}y\,dy=164041/1640160. For r≥1r\geq 1, Jensen’s inequality for y↦(r/5+y)−2y\mapsto(r/5+y)^{-2} gives

∑k(1r/5+ak−1r/5+bk)=∑k∫akbkd⁢y(r/5+y)2≥ℓ(r/5+y¯)2.\sum_{k}\Bigl{(}\frac{1}{r/5+a_{k}}-\frac{1}{r/5+b_{k}}\Bigr{)}=\sum_{k}\int_{% a_{k}}^{b_{k}}\frac{dy}{(r/5+y)^{2}}\geq\frac{\ell}{(r/5+\bar{y})^{2}}.

So the intervals with 1≤r≤91\leq r\leq 9 contribute at least ℓ40⁢∑r(r/5+y¯)−2>0.0260\frac{\ell}{40}\sum_{r}(r/5+\bar{y})^{-2}>0.0260 (Table B.1). The intervals ℰi\mathcal{E}_{i} contribute 20200739891364696932300>3.1223\frac{202007398913}{64696932300}>3.1223. Thus δ>1.6187+0.0260+3.1223=4.7670\delta>1.6187+0.0260+3.1223=4.7670. ∎

5. Analytic estimates

5.1. The double integral

Write JN(0)J_{N}^{(0)}, JN(1)J_{N}^{(1)} for J4(0)J_{4}^{(0)}, J4(1)J_{4}^{(1)} at the tuple (1.1).

Lemma 5.1.

Let y=η/(η−4)y=\eta/(\eta-4). Then R4⁢(x,y)⁢d⁢y=−fN⁢(x,η)⁢d⁢ηR_{4}(x,y)\,dy=-f_{N}(x,\eta)\,d\eta, where

fN⁢(x,η)=Ψ⁢(x,η)N(x−η)⁢(4−η),Ψ⁢(x,η)=x240⁢(1−x)240⁢η190⁢(1−η)190(x−η)215⁢(4−η)322.f_{N}(x,\eta)=\frac{\Psi(x,\eta)^{N}}{(x-\eta)(4-\eta)},\qquad\Psi(x,\eta)=% \frac{x^{240}(1-x)^{240}\,\eta^{190}(1-\eta)^{190}}{(x-\eta)^{215}(4-\eta)^{32% 2}}.

In particular, with

Φ⁢(x,τ)=Ψ⁢(x,−τ)=x240⁢(1−x)240⁢τ190⁢(1+τ)190(x+τ)215⁢(4+τ)322,\Phi(x,\tau)=\Psi(x,-\tau)=\frac{x^{240}(1-x)^{240}\,\tau^{190}(1+\tau)^{190}}% {(x+\tau)^{215}(4+\tau)^{322}},

we have

JN(0)=∫01∫0∞Φ⁢(x,τ)N(x+τ)⁢(4+τ)⁢𝑑τ⁢𝑑x.J_{N}^{(0)}=\int_{0}^{1}\!\!\int_{0}^{\infty}\frac{\Phi(x,\tau)^{N}}{(x+\tau)(% 4+\tau)}\,d\tau\,dx.
Proof.

We have

y=−η4−η,1−y=44−η,1+3⁢y=4⁢(1−η)4−η,\displaystyle y=\frac{-\eta}{4-\eta},\qquad 1-y=\frac{4}{4-\eta},\qquad 1+3y=% \frac{4(1-\eta)}{4-\eta},
x⁢(1−y)+4⁢y=4⁢(x−η)4−η,d⁢y=−4⁢d⁢η(4−η)2.\displaystyle x(1-y)+4y=\frac{4(x-\eta)}{4-\eta},\qquad dy=\frac{-4\,d\eta}{(4% -\eta)^{2}}.

The exponents are j=h=240⁢Nj=h=240N, k=190⁢Nk=190N, l=157⁢Nl=157N, j+q−m=190⁢Nj+q-m=190N, j+k−m+1=215⁢N+1j+k-m+1=215N+1 and k−l−q=−132⁢Nk-l-q=-132N. The powers of 44 cancel, since −132+157+190−215=0-132+157+190-215=0 and 4−1⋅4=14^{-1}\cdot 4=1. Those of 4−η4-\eta add to −(322⁢N+1)-(322N+1), and (−η)190⁢N=η190⁢N(-\eta)^{190N}=\eta^{190N}. For JN(0)J_{N}^{(0)} put τ=−η\tau=-\eta. Then τ\tau runs over [0,∞)[0,\infty) as yy runs over [0,1)[0,1), and −fN⁢d⁢η=fN⁢(x,−τ)⁢d⁢τ-f_{N}\,d\eta=f_{N}(x,-\tau)\,d\tau. ∎

Lemma 5.2.

For N≥1N\geq 1, 10−9⁢e−40⁢(18.88)⁢N<JN(0)<e−40⁢(18.87333)⁢N10^{-9}e^{-40(18.88)N}<J_{N}^{(0)}<e^{-40(18.87333)N}.

Proof.

Weighted AM–GM, x+τ≥215⁢(x/25)25/215⁢(τ/190)190/215x+\tau\geq 215\,(x/25)^{25/215}(\tau/190)^{190/215}, gives

Φ\displaystyle\Phi ≤(543)25⁢(3843)190⁢x215⁢(1−x)240⁢(1+τ)190(4+τ)322\displaystyle\leq\Bigl{(}\frac{5}{43}\Bigr{)}^{25}\Bigl{(}\frac{38}{43}\Bigr{)% }^{190}x^{215}(1-x)^{240}\,\frac{(1+\tau)^{190}}{(4+\tau)^{322}}
≤Φ+:=(543)25⁢(3843)190⁢(4391)215⁢(4891)240⁢(95/22)190(161/22)322,\displaystyle\leq\Phi_{+}:=\Bigl{(}\frac{5}{43}\Bigr{)}^{25}\Bigl{(}\frac{38}{% 43}\Bigr{)}^{190}\Bigl{(}\frac{43}{91}\Bigr{)}^{215}\Bigl{(}\frac{48}{91}\Bigr% {)}^{240}\frac{(95/22)^{190}}{(161/22)^{322}},

with maxima at x=43/91x=43/91 and τ=73/22\tau=73/22. By Table B.1, −log⁡Φ+>40⁢(18.87333)-\log\Phi_{+}>40(18.87333). Also

∫01∫0∞d⁢τ⁢d⁢x(x+τ)⁢(4+τ)=∫01log⁡(4/x)4−x⁢𝑑x<1+log⁡43<1,\int_{0}^{1}\!\!\int_{0}^{\infty}\frac{d\tau\,dx}{(x+\tau)(4+\tau)}=\int_{0}^{% 1}\frac{\log(4/x)}{4-x}\,dx<\frac{1+\log 4}{3}<1,

so JN(0)<Φ+NJ_{N}^{(0)}<\Phi_{+}^{N}. For the lower bound let ℬ=[0.4711,0.4713]×[3.3999,3.4001]\mathcal{B}=[0.4711,0.4713]\times[3.3999,3.4001]. Bounding each factor of Φ\Phi by its least value on ℬ\mathcal{B} gives

Φ≥Φ−:=0.4711240⁢ 0.5287240⁢ 3.3999190⁢ 4.39991903.8714215⁢ 7.4001322on ⁢ℬ,\Phi\geq\Phi_{-}:=\frac{0.4711^{240}\,0.5287^{240}\,3.3999^{190}\,4.3999^{190}% }{3.8714^{215}\,7.4001^{322}}\qquad\text{on }\mathcal{B},

and (x+τ)⁢(4+τ)<29(x+\tau)(4+\tau)<29 there. By Table B.1, −log⁡Φ−<40⁢(18.88)-\log\Phi_{-}<40(18.88). Hence JN(0)≥area⁡(ℬ)⁢Φ−N/29=4⋅10−8⁢Φ−N/29>10−9⁢e−40⁢(18.88)⁢NJ_{N}^{(0)}\geq\operatorname{area}(\mathcal{B})\,\Phi_{-}^{N}/29=4\cdot 10^{-8% }\,\Phi_{-}^{N}/29>10^{-9}e^{-40(18.88)N}. ∎

5.2. The residue integral

Put A=(3+4⁢i)/5A=(3+4i)/5, B=(5−12⁢i)/13B=(5-12i)/13 and, for 0≤t,u≤10\leq t,u\leq 1,

X⁢(t)=tt+A⁢(1−t),Y⁢(u)=uu+B⁢(1−u),ω=t⁢(1−u)+u⁢(1−t).X(t)=\frac{t}{t+A(1-t)},\qquad Y(u)=\frac{u}{u+B(1-u)},\qquad\omega=t(1-u)+u(1% -t).
Lemma 5.3.

For 0≤t,u≤10\leq t,u\leq 1 and x∈[0,1]x\in[0,1]:

  1. (1)

    |X′|≤5/4|X^{\prime}|\leq 5/4, |Y′|≤13/9|Y^{\prime}|\leq 13/9, |X⁢(1−X)|≤54⁢t⁢(1−t)≤54⁢ω|X(1-X)|\leq\frac{5}{4}t(1-t)\leq\frac{5}{4}\omega, |Y⁢(1−Y)|≤139⁢u⁢(1−u)≤139⁢ω|Y(1-Y)|\leq\frac{13}{9}u(1-u)\leq\frac{13}{9}\omega, |Y|≤1|Y|\leq 1 and |4−Y|≥3|4-Y|\geq 3;

  2. (2)

    |X−Y|≥7⁢ω/65|X-Y|\geq 7\omega/\sqrt{65}, and |x−Y|≥2⁢ωx/13|x-Y|\geq 2\omega_{x}/\sqrt{13} with ωx=x⁢(1−u)+u⁢(1−x)\omega_{x}=x(1-u)+u(1-x);

  3. (3)

    Im⁡X⁢(t)<0<Im⁡Y⁢(u)\operatorname{Im}X(t)<0<\operatorname{Im}Y(u) for 0<t,u<10<t,u<1.

Proof.

One has |t+A⁢(1−t)|2=1−45⁢t⁢(1−t)≥45|t+A(1-t)|^{2}=1-\frac{4}{5}t(1-t)\geq\frac{4}{5}, |u+B⁢(1−u)|2=1−1613⁢u⁢(1−u)≥913|u+B(1-u)|^{2}=1-\frac{16}{13}u(1-u)\geq\frac{9}{13}, X′=A/(t+A⁢(1−t))2X^{\prime}=A/(t+A(1-t))^{2} and 1−X=A⁢(1−t)/(t+A⁢(1−t))1-X=A(1-t)/(t+A(1-t)); similarly for YY. Also |u+B⁢(1−u)|2−u2=(1−u)⁢(13−3⁢u)/13≥0|u+B(1-u)|^{2}-u^{2}=(1-u)(13-3u)/13\geq 0, so |Y|≤1|Y|\leq 1. Next t⁢(1−t)≤ωt(1-t)\leq\omega, since ω−t⁢(1−t)\omega-t(1-t) equals u⁢(1−2⁢t)+t2≥0u(1-2t)+t^{2}\geq 0 for t≤12t\leq\frac{1}{2} and is at least (1−t)2(1-t)^{2} for t≥12t\geq\frac{1}{2}; likewise u⁢(1−u)≤ωu(1-u)\leq\omega. For (2), X−Y=t⁢B⁢(1−u)−u⁢A⁢(1−t)(t+A⁢(1−t))⁢(u+B⁢(1−u))X-Y=\frac{tB(1-u)-uA(1-t)}{(t+A(1-t))(u+B(1-u))} and the denominator has modulus at most 11. With ξ=t⁢(1−u)\xi=t(1-u), ζ=u⁢(1−t)\zeta=u(1-t) and γ=Re⁡(B⁢A¯)=−33/65\gamma=\operatorname{Re}(B\bar{A})=-33/65,

|t⁢B⁢(1−u)−u⁢A⁢(1−t)|2=ξ2+ζ2−2⁢γ⁢ξ⁢ζ=1−γ2⁢ω2+1+γ2⁢(ξ−ζ)2≥4965⁢ω2.|tB(1-u)-uA(1-t)|^{2}=\xi^{2}+\zeta^{2}-2\gamma\xi\zeta=\tfrac{1-\gamma}{2}\,% \omega^{2}+\tfrac{1+\gamma}{2}(\xi-\zeta)^{2}\geq\tfrac{49}{65}\,\omega^{2}.

For real xx take A=1A=1, t=xt=x and γ=Re⁡B=5/13\gamma=\operatorname{Re}B=5/13. Part (3) follows from Im⁡X=−45⁢t⁢(1−t)/|t+A⁢(1−t)|2\operatorname{Im}X=-\frac{4}{5}t(1-t)/|t+A(1-t)|^{2} and its analogue. ∎

Lemma 5.4.

For N≥1N\geq 1, JN(1)=π−1⁢Im⁡ZNJ_{N}^{(1)}=\pi^{-1}\operatorname{Im}Z_{N}, where

ZN=∫01∫01fN⁢(X⁢(t),Y⁢(u))⁢X′⁢(t)⁢Y′⁢(u)⁢𝑑t⁢𝑑u.Z_{N}=\int_{0}^{1}\!\!\int_{0}^{1}f_{N}\bigl{(}X(t),Y(u)\bigr{)}\,X^{\prime}(t% )\,Y^{\prime}(u)\,dt\,du.
Proof.

Residues are invariant under the change of variables of Lemma 5.1, and y=x/(x−4)y=x/(x-4) corresponds to η=x\eta=x. Hence JN(1)=−∫01Resη=xfN⁢(x,η)⁢𝑑xJ_{N}^{(1)}=-\int_{0}^{1}\operatorname*{Res}_{\eta=x}f_{N}(x,\eta)\,dx. Fix x∈(0,1)x\in(0,1). By Lemma 5.3, YY runs from 0 to 11 in the upper half-plane and Y¯\bar{Y} in the lower one, both in the closed unit disc. So Y¯\bar{Y} followed by YY reversed is a positively oriented Jordan curve around xx, and the other pole η=4\eta=4 lies outside. As fNf_{N} has real coefficients, the residue theorem gives

Resη=xfN=W⁢(x)¯−W⁢(x)2⁢π⁢i=−Im⁡W⁢(x)π,W⁢(x)=∫01fN⁢(x,Y⁢(u))⁢Y′⁢(u)⁢𝑑u.\operatorname*{Res}_{\eta=x}f_{N}=\frac{\overline{W(x)}-W(x)}{2\pi i}=-\frac{% \operatorname{Im}W(x)}{\pi},\qquad W(x)=\int_{0}^{1}f_{N}(x,Y(u))\,Y^{\prime}(% u)\,du.

By Lemma 5.3, also with tt replaced by xx,

|fN⁢(x,Y)⁢Y′|≪Nωx215⁢N−1,|fN⁢(X,Y)⁢X′⁢Y′|≪Nω215⁢N−1,|f_{N}(x,Y)\,Y^{\prime}|\ll_{N}\omega_{x}^{215N-1},\qquad|f_{N}(X,Y)\,X^{% \prime}Y^{\prime}|\ll_{N}\omega^{215N-1},

so both are bounded on [0,1]2[0,1]^{2}. For fixed u∈(0,1)u\in(0,1) the function w↦fN⁢(w,Y⁢(u))w\mapsto f_{N}(w,Y(u)) is holomorphic off w=Y⁢(u)w=Y(u), and Im⁡Y⁢(u)>0≥Im⁡X⁢(t)\operatorname{Im}Y(u)>0\geq\operatorname{Im}X(t). Cauchy’s theorem moves ∫01𝑑x\int_{0}^{1}dx to the arc XX, and Fubini’s theorem gives ∫01W⁢(x)⁢𝑑x=ZN\int_{0}^{1}W(x)\,dx=Z_{N}. ∎

Lemma 5.5.

For N≥1N\geq 1, |JN(1)|<e−40⁢(18.8995)⁢N|J_{N}^{(1)}|<e^{-40(18.8995)N}.

Proof.

Put r=t/(1−t)=eRr=t/(1-t)=e^{R} and s=u/(1−u)=eSs=u/(1-u)=e^{S}, so X=r/(r+A)X=r/(r+A) and Y=s/(s+B)Y=s/(s+B). With

Q1=r2+65⁢r+1,Q2=s2+1013⁢s+1,Q3=r2+6665⁢r⁢s+s2,Q4=9⁢s2+12013⁢s+16,Q_{1}=r^{2}+\tfrac{6}{5}r+1,\quad Q_{2}=s^{2}+\tfrac{10}{13}s+1,\quad Q_{3}=r^% {2}+\tfrac{66}{65}rs+s^{2},\quad Q_{4}=9s^{2}+\tfrac{120}{13}s+16,

one has |X⁢(1−X)|=r/Q1|X(1-X)|=r/Q_{1}, |Y⁢(1−Y)|=s/Q2|Y(1-Y)|=s/Q_{2}, |X−Y|2=Q3/(Q1⁢Q2)|X-Y|^{2}=Q_{3}/(Q_{1}Q_{2}) and |4−Y|2=Q4/Q2|4-Y|^{2}=Q_{4}/Q_{2}. So log⁡|Ψ⁢(X,Y)|=L\log|\Psi(X,Y)|=L, where

L=240⁢log⁡r+190⁢log⁡s−2652⁢log⁡Q1+1572⁢log⁡Q2−2152⁢log⁡Q3−161⁢log⁡Q4.L=240\log r+190\log s-\tfrac{265}{2}\log Q_{1}+\tfrac{157}{2}\log Q_{2}-\tfrac% {215}{2}\log Q_{3}-161\log Q_{4}.

Let ℓγ⁢(v)=log⁡(cosh⁡v+γ)\ell_{\gamma}(v)=\log(\cosh v+\gamma) and κ=log⁡(4/3)\kappa=\log(4/3). Since Q1=2⁢r⁢(cosh⁡R+35)Q_{1}=2r(\cosh R+\frac{3}{5}), Q2=2⁢s⁢(cosh⁡S+513)Q_{2}=2s(\cosh S+\frac{5}{13}), Q3=2⁢r⁢s⁢(cosh⁡(R−S)+3365)Q_{3}=2rs(\cosh(R-S)+\frac{33}{65}) and Q4=24⁢s⁢(cosh⁡(S−κ)+513)Q_{4}=24s(\cosh(S-\kappa)+\frac{5}{13}),

L=\displaystyle L={} −3232⁢log⁡2−161⁢log⁡24−2652⁢ℓ3/5⁢(R)+1572⁢ℓ5/13⁢(S)\displaystyle-\tfrac{323}{2}\log 2-161\log 24-\tfrac{265}{2}\ell_{3/5}(R)+% \tfrac{157}{2}\ell_{5/13}(S)
−2152⁢ℓ33/65⁢(R−S)−161⁢ℓ5/13⁢(S−κ).\displaystyle-\tfrac{215}{2}\ell_{33/65}(R-S)-161\,\ell_{5/13}(S-\kappa).

Here ℓγ′′=(1+γ⁢cosh⁡v)/(cosh⁡v+γ)2>0\ell_{\gamma}^{\prime\prime}=(1+\gamma\cosh v)/(\cosh v+\gamma)^{2}>0 and, for 0<γ<10<\gamma<1,

(log⁡ℓγ′′)′=−sinh⁡v⁢2+γ⁢cosh⁡v−γ2(1+γ⁢cosh⁡v)⁢(cosh⁡v+γ),|(log⁡ℓγ′′)′|≤2⁢|sinh⁡v|cosh⁡v+γ<2,(\log\ell_{\gamma}^{\prime\prime})^{\prime}=-\sinh v\,\frac{2+\gamma\cosh v-% \gamma^{2}}{(1+\gamma\cosh v)(\cosh v+\gamma)},\qquad|(\log\ell_{\gamma}^{% \prime\prime})^{\prime}|\leq\frac{2|\sinh v|}{\cosh v+\gamma}<2,

so ℓγ′′⁢(v−κ)≥916⁢ℓγ′′⁢(v)\ell_{\gamma}^{\prime\prime}(v-\kappa)\geq\frac{9}{16}\ell_{\gamma}^{\prime% \prime}(v). Therefore

−d2⁢L=\displaystyle-d^{2}L={} 2652⁢ℓ3/5′′⁢(R)⁢d⁢R2+2152⁢ℓ33/65′′⁢(R−S)⁢(d⁢R−d⁢S)2\displaystyle\tfrac{265}{2}\ell_{3/5}^{\prime\prime}(R)\,dR^{2}+\tfrac{215}{2}% \ell_{33/65}^{\prime\prime}(R-S)(dR-dS)^{2}
+(161⁢ℓ5/13′′⁢(S−κ)−1572⁢ℓ5/13′′⁢(S))⁢d⁢S2\displaystyle+\bigl{(}161\,\ell_{5/13}^{\prime\prime}(S-\kappa)-\tfrac{157}{2}% \ell_{5/13}^{\prime\prime}(S)\bigr{)}dS^{2}

is positive definite, since 161⋅916>1572161\cdot\frac{9}{16}>\frac{157}{2}. So LL is strictly concave and LR⁢S>0L_{RS}>0. The partial derivatives are

LR\displaystyle L_{R} =240−265⁢r⁢(r+3/5)Q1−215⁢r⁢(r+33⁢s/65)Q3,\displaystyle=240-265\,\frac{r(r+3/5)}{Q_{1}}-215\,\frac{r(r+33s/65)}{Q_{3}},
LS\displaystyle L_{S} =190+157⁢s⁢(s+5/13)Q2−215⁢s⁢(s+33⁢r/65)Q3−322⁢s⁢(9⁢s+60/13)Q4.\displaystyle=190+157\,\frac{s(s+5/13)}{Q_{2}}-215\,\frac{s(s+33r/65)}{Q_{3}}-% 322\,\frac{s(9s+60/13)}{Q_{4}}.

Table B.2 gives LR,LS>0L_{R},L_{S}>0 at (r,s)=(2925,139100)(r,s)=(\frac{29}{25},\frac{139}{100}) and LR,LS<0L_{R},L_{S}<0 at (5950,7150)(\frac{59}{50},\frac{71}{50}). Consider the box 2925≤r≤5950\frac{29}{25}\leq r\leq\frac{59}{50}, 139100≤s≤7150\frac{139}{100}\leq s\leq\frac{71}{50}. Since LR⁢S>0L_{RS}>0, we get LR>0L_{R}>0 on its face r=2925r=\frac{29}{25}, LR<0L_{R}<0 on r=5950r=\frac{59}{50}, LS>0L_{S}>0 on s=139100s=\frac{139}{100} and LS<0L_{S}<0 on s=7150s=\frac{71}{50}. So the maximum of LL on the box is an interior critical point, hence the global maximum. At (r,s)=(117100,75)(r,s)=(\frac{117}{100},\frac{7}{5}), Table B.2 gives −14<LR<0<LS<310-\frac{1}{4}<L_{R}<0<L_{S}<\frac{3}{10} and L<−755.99L<-755.99. Concavity gives

supL<−755.99+14⁢log⁡117116+310⁢log⁡7170<−755.99+1464+3700<−755.98.\sup L<-755.99+\tfrac{1}{4}\log\tfrac{117}{116}+\tfrac{3}{10}\log\tfrac{71}{70% }<-755.99+\tfrac{1}{464}+\tfrac{3}{700}<-755.98.

By Lemma 5.3, |X′⁢Y′|<2|X^{\prime}Y^{\prime}|<2, |X−Y|≥45⁢ω|X-Y|\geq\frac{4}{5}\omega and |4−Y|≥3|4-Y|\geq 3. With w=1−2⁢uw=1-2u,

∫01∫01d⁢t⁢d⁢uω=∫01log⁡1−uu1−2⁢u⁢𝑑u=12⁢∫−11log⁡1+w1−w⁢d⁢ww=2⁢∑n≥01(2⁢n+1)2=π24.\int_{0}^{1}\!\!\int_{0}^{1}\frac{dt\,du}{\omega}=\int_{0}^{1}\frac{\log\frac{% 1-u}{u}}{1-2u}\,du=\frac{1}{2}\int_{-1}^{1}\log\frac{1+w}{1-w}\,\frac{dw}{w}=2% \sum_{n\geq 0}\frac{1}{(2n+1)^{2}}=\frac{\pi^{2}}{4}.

By Lemma 5.4,

|JN(1)|≤1π⋅2⋅54⋅13⋅π24⁢e−40⁢(18.8995)⁢N=5⁢π24⁢e−40⁢(18.8995)⁢N<e−40⁢(18.8995)⁢N.∎|J_{N}^{(1)}|\leq\frac{1}{\pi}\cdot 2\cdot\frac{5}{4}\cdot\frac{1}{3}\cdot% \frac{\pi^{2}}{4}\,e^{-40(18.8995)N}=\frac{5\pi}{24}\,e^{-40(18.8995)N}<e^{-40% (18.8995)N}.\qed

6. Proof of Theorem 1

By Lemmas 5.2 and 5.5, JN(0)>10−9⁢e−40⁢(18.88)⁢N>(log⁡4)⁢|JN(1)|J_{N}^{(0)}>10^{-9}e^{-40(18.88)N}>(\log 4)\,|J_{N}^{(1)}| for large NN. Hence GN=JN(0)−(log⁡4)⁢JN(1)>0G_{N}=J_{N}^{(0)}-(\log 4)J_{N}^{(1)}>0 and GN<3⁢e−40⁢(18.87333)⁢NG_{N}<3e^{-40(18.87333)N}. Put

ΛN=DNΔN⁢GN=DNΔN⁢c1⁢(GN)−DNΔN⁢c2⁢(GN)⁢θ.\Lambda_{N}=\frac{D_{N}}{\Delta_{N}}\,G_{N}=\frac{D_{N}}{\Delta_{N}}\,c_{1}(G_% {N})-\frac{D_{N}}{\Delta_{N}}\,c_{2}(G_{N})\,\theta.

By (3.1) and Lemma 4.1, ΛN∈ℤ+ℤ⁢θ\Lambda_{N}\in\mathbb{Z}+\mathbb{Z}\theta. Also ΛN>0\Lambda_{N}>0 for large NN, and

lim supN→∞log⁡ΛN40⁢N≤cD−δ−18.87333<23.63856−4.7670−18.87333=−0.00177.\limsup_{N\to\infty}\frac{\log\Lambda_{N}}{40N}\leq c_{D}-\delta-18.87333<23.6% 3856-4.7670-18.87333=-0.00177.

If q0⁢θ∈ℤq_{0}\theta\in\mathbb{Z} for an integer q0≥1q_{0}\geq 1, then q0⁢ΛNq_{0}\Lambda_{N} is a positive integer for large NN and q0⁢ΛN→0q_{0}\Lambda_{N}\to 0, which is impossible. ∎

Appendix A Floor data

Table A.1 cuts each ℰi\mathcal{E}_{i} at the jumps of the FaF_{a}. On each piece, Fa=⌊a⁢x0⌋F_{a}=\lfloor ax_{0}\rfloor with x0x_{0} the left end. The columns CC, UbU_{b}, VbV_{b} follow from Lemma 3.2, and the last column is 1+[C=1]1+[\,C=1\,]. The first row uses (2.2) instead of CC, UbU_{b}, VbV_{b}.

Table A.1. Floors on the pieces of ℰ1,…,ℰ18\mathcal{E}_{1},\dots,\mathcal{E}_{18}.
piece F157F_{157} F190F_{190} F215F_{215} F240F_{240} F265F_{265} F322F_{322} F323F_{323} CC U190U_{190} U215U_{215} V190V_{190} V215V_{215} 1+[C=1]1{+}[\,C{=}1\,]
(1/322,1/265)(1/322,1/265) 0 0 0 0 0 11 11 by (2.2) 11
(1/215,1/190)(1/215,1/190) 0 0 11 11 11 11 11 0 −1-1 11 −2-2 0 11
[1/190,2/323)[1/190,2/323) 0 11 11 11 11 11 11 0 11 11 0 0 11
(2/215,3/322)(2/215,3/322) 11 11 22 22 22 22 33 0 −1-1 11 −1-1 11 11
(3/215,4/265)(3/215,4/265) 22 22 33 33 33 44 44 0 −1-1 11 −1-1 11 11
(4/190,7/323)(4/190,7/323) 33 44 44 55 55 66 66 11 22 11 11 0 22
(7/265,9/323)(7/265,9/323) 44 55 55 66 77 88 88 0 11 −1-1 11 −1-1 11
[9/323,6/215)[9/323,6/215) 44 55 55 66 77 88 99 0 0 −2-2 11 −1-1 11
[6/215,9/322)[6/215,9/322) 44 55 66 66 77 88 99 −1-1 −1-1 0 0 11 11
(5/157,7/215)(5/157,7/215) 55 66 66 77 88 1010 1010 0 0 −2-2 11 −1-1 11
[7/215,8/240)[7/215,8/240) 55 66 77 77 88 1010 1010 −1-1 −1-1 0 0 11 11
[8/240,9/265)[8/240,9/265) 55 66 77 88 88 1010 1010 11 11 22 0 11 22
[9/265,11/323)[9/265,11/323) 55 66 77 88 99 1010 1010 0 11 11 0 0 11
(7/190,12/323)(7/190,12/323) 55 77 77 88 99 1111 1111 0 11 −1-1 11 −1-1 11
[12/323,8/215)[12/323,8/215) 55 77 77 88 99 1111 1212 0 0 −2-2 11 −1-1 11
[8/215,12/322)[8/215,12/322) 55 77 88 88 99 1111 1212 −1-1 −1-1 0 0 11 11
(9/215,8/190)(9/215,8/190) 66 77 99 1010 1111 1313 1313 0 −1-1 11 −2-2 0 11
[8/190,14/323)[8/190,14/323) 66 88 99 1010 1111 1313 1313 0 11 11 0 0 11
(11/215,10/190)(11/215,10/190) 88 99 1111 1212 1313 1616 1616 0 −1-1 11 −1-1 11 11
[10/190,17/322)[10/190,17/322) 88 1010 1111 1212 1313 1616 1717 0 0 0 11 11 11
(11/190,14/240)(11/190,14/240) 99 1111 1212 1313 1515 1818 1818 −1-1 0 −1-1 11 0 11
[14/240,19/323)[14/240,19/323) 99 1111 1212 1414 1515 1818 1818 11 22 11 11 0 22
(17/265,21/323)(17/265,21/323) 1010 1212 1313 1515 1717 2020 2020 0 11 −1-1 11 −1-1 11
[21/323,14/215)[21/323,14/215) 1010 1212 1313 1515 1717 2020 2121 0 0 −2-2 11 −1-1 11
[14/215,21/322)[14/215,21/322) 1010 1212 1414 1515 1717 2020 2121 −1-1 −1-1 0 0 11 11
(11/157,17/240)(11/157,17/240) 1111 1313 1515 1616 1818 2222 2222 −1-1 −1-1 0 0 11 11
[17/240,23/323)[17/240,23/323) 1111 1313 1515 1717 1818 2222 2222 11 11 22 0 11 22
(14/190,24/323)(14/190,24/323) 1111 1414 1515 1717 1919 2323 2323 0 11 −1-1 11 −1-1 11
[24/323,16/215)[24/323,16/215) 1111 1414 1515 1717 1919 2323 2424 0 0 −2-2 11 −1-1 11
[16/215,24/322)[16/215,24/322) 1111 1414 1616 1717 1919 2323 2424 −1-1 −1-1 0 0 11 11
(15/190,17/215)(15/190,17/215) 1212 1515 1616 1818 2020 2525 2525 0 0 −2-2 11 −1-1 11
[17/215,19/240)[17/215,19/240) 1212 1515 1717 1818 2020 2525 2525 −1-1 −1-1 0 0 11 11
[19/240,21/265)[19/240,21/265) 1212 1515 1717 1919 2020 2525 2525 11 11 22 0 11 22
[21/265,26/323)[21/265,26/323) 1212 1515 1717 1919 2121 2525 2525 0 11 11 0 0 11
(19/215,14/157)(19/215,14/157) 1313 1616 1919 2121 2323 2828 2828 0 −1-1 11 −2-2 0 11
[14/157,17/190)[14/157,17/190) 1414 1616 1919 2121 2323 2828 2828 0 −1-1 11 −1-1 11 11
[17/190,29/323)[17/190,29/323) 1414 1717 1919 2121 2323 2828 2828 0 11 11 11 11 11
[29/323,29/322)[29/323,29/322) 1414 1717 1919 2121 2323 2828 2929 0 0 0 11 11 11
(21/190,36/323)(21/190,36/323) 1717 2121 2323 2626 2929 3535 3535 0 11 −1-1 11 −1-1 11
[36/323,24/215)[36/323,24/215) 1717 2121 2323 2626 2929 3535 3636 0 0 −2-2 11 −1-1 11
[24/215,36/322)[24/215,36/322) 1717 2121 2424 2626 2929 3535 3636 −1-1 −1-1 0 0 11 11
(22/190,25/215)(22/190,25/215) 1818 2222 2424 2727 3030 3737 3737 0 0 −2-2 11 −1-1 11
[25/215,28/240)[25/215,28/240) 1818 2222 2525 2727 3030 3737 3737 −1-1 −1-1 0 0 11 11
[28/240,31/265)[28/240,31/265) 1818 2222 2525 2828 3030 3737 3737 11 11 22 0 11 22
[31/265,38/323)[31/265,38/323) 1818 2222 2525 2828 3131 3737 3737 0 11 11 0 0 11
Table A.2. The two cases in the definition of bkb_{k}.
jkj_{k} ϱk≤21\varrho_{k}\leq 21 k−jkk-j_{k} ϱk≥22\varrho_{k}\geq 22 k+jk+1k+j_{k}+1
0 1≤k≤41\leq k\leq 4 1,…,41,\dots,4 5≤k≤95\leq k\leq 9 6,…,106,\dots,10
1 10≤k≤1310\leq k\leq 13 9,…,129,\dots,12 14≤k≤1914\leq k\leq 19 16,…,2116,\dots,21
2 20≤k≤2320\leq k\leq 23 18,…,2118,\dots,21 24≤k≤2824\leq k\leq 28 27,…,3127,\dots,31
3 29≤k≤3329\leq k\leq 33 26,…,3026,\dots,30 34≤k≤3834\leq k\leq 38 38,…,4238,\dots,42
4 39≤k≤4239\leq k\leq 42 35,…,3835,\dots,38 43≤k≤4743\leq k\leq 47 48,…,5248,\dots,52

Appendix B Numerical values

Values are truncated to the digits shown.

Table B.1. Constants.
quantity value
−log⁡Φ+/40-\log\Phi_{+}/40 18.8733376741⁢…18.8733376741\ldots
−log⁡Φ−/40-\log\Phi_{-}/40 18.8775167011⁢…18.8775167011\ldots
cDc_{D} 23.6385592638⁢…23.6385592638\ldots
δ0\delta_{0} 1.6187800851⁢…1.6187800851\ldots
ℓ40⁢∑r=19(r/5+y¯)−2\frac{\ell}{40}\sum_{r=1}^{9}(r/5+\bar{y})^{-2} 0.0260767666⁢…0.0260767666\ldots
140⁢∑i∫ℰix−2⁢𝑑x\frac{1}{40}\sum_{i}\int_{\mathcal{E}_{i}}x^{-2}\,dx 3.1223644109⁢…3.1223644109\ldots
Table B.2. Values of LRL_{R}, LSL_{S} and LL.
(r,s)(r,s) LRL_{R} LSL_{S} LL
(29/25, 139/100)(29/25,\,139/100) 0.57635⁢…0.57635\ldots 0.62026⁢…0.62026\ldots
(59/50, 71/50)(59/50,\,71/50) −0.52544⁢…-0.52544\ldots −1.02457⁢…-1.02457\ldots
(117/100, 7/5)(117/100,\,7/5) −0.22659⁢…-0.22659\ldots 0.26833⁢…0.26833\ldots −755.99795⁢…-755.99795\ldots

Appendix C Computer checks

The two scripts in Table C.1 recheck only the statements listed there, in exact rational arithmetic. They are included as ancillary files. The proof does not use them. For log⁡v\log v the analytic script writes v=2e⁢qv=2^{e}q with e∈ℤe\in\mathbb{Z}, 1≤q≤21\leq q\leq 2, and uses 3030 terms of log⁡q=2⁢∑n≥0w2⁢n+1/(2⁢n+1)\log q=2\sum_{n\geq 0}w^{2n+1}/(2n+1), w=(q−1)/(q+1)w=(q-1)/(q+1), with tail at most 2⁢w61/(61⁢(1−w2))2w^{61}/(61(1-w^{2})).

Table C.1. Scripts.
script statements checked time
check_arith.py the intervals ℰi\mathcal{E}_{i} and Tables A.1, A.2 as printed; Lemma 3.3; the tuples s1,s2,s3,s′s_{1},s_{2},s_{3},s^{\prime} and the floor sums in Lemma 3.2; Proposition 3.4 for 1/265≤x<21/265\leq x<2 at each jump of the FaF_{a} and between consecutive jumps, and M=0M=0, μ=1\mu=1 on ℰ1\mathcal{E}_{1}; the numbers in Lemma 4.1; 57/4057/40 and 3.353.35 in Section 1; rows 4–6 of Table B.1 10 s
check_arith.py --brute 1,2,3,4,5,6,7,8 for N≤8N\leq 8 and all primes pp with 3<p≤323⁢N3<p\leq 323N and p2>430⁢Np^{2}>430N (for larger pp, μ⁢(N/p)=0\mu(N/p)=0), the best bound from Lemma 3.1 over (2.1) with b=190,215b=190,215 and (2.2), all λ\lambda and all s∈O⁢(t)s\in O(t), is at least μ⁢(N/p)\mu(N/p) 3 min
check_analytic.py the exponents in Lemma 5.1; the constants in Lemma 5.2; the identities in Lemmas 5.3 and 5.5 at rational points; rows 1–3 of Table B.1 and Table B.2 as printed; 23.63856−4.7670−18.87333=−0.0017723.63856-4.7670-18.87333=-0.00177 1 s

Use of AI tools

Codex (OpenAI, GPT-5.6 Sol) searched for the parameters in (1.1) and wrote the Python code and the interval lists. Claude Code (Anthropic, Claude Fable 5) checked the code, the parameters and the tables. The author checked every step of the proof, every table and every reference, and takes full responsibility for the content of the paper.

References

  • [1] F. Calegari, V. Dimitrov, and Y. Tang, The linear independence of 11, ζ⁢(2)\zeta(2), and L⁢(2,χ−3)L(2,\chi_{-3}), preprint (2024), arXiv:2408.15403v2.
  • [2] NIST Digital Library of Mathematical Functions, https://dlmf.nist.gov/, Release 1.2.8 of 2026-09-15, F. W. J. Olver et al., eds.
  • [3] M. Hata, Rational approximations to the dilogarithm, Trans. Amer. Math. Soc. 336 (1993), no. 1, 363–387. MR1147401
  • [4] T. Prellberg, Three irrationality results for the dilogarithm: Rhin–Viola and Viola–Zudilin constructions at −1/4-1/4, 1/51/5, and −1/3-1/3, preprint (2026), arXiv:2609.06895v1.
  • [5] G. Rhin and C. Viola, On a permutation group related to ζ⁢(2)\zeta(2), Acta Arith. 77 (1996), no. 1, 23–56. MR1404975
  • [6] G. Rhin and C. Viola, The permutation group method for the dilogarithm, Ann. Sc. Norm. Super. Pisa Cl. Sci. (5) 4 (2005), no. 3, 389–437. MR2185863
  • [7] G. Rhin and C. Viola, Linear independence of 11, Li1\mathrm{Li}_{1} and Li2\mathrm{Li}_{2}, Mosc. J. Comb. Number Theory 8 (2019), no. 1, 81–96. MR3864310
  • [8] C. Viola and W. Zudilin, Linear independence of dilogarithmic values, J. Reine Angew. Math. 736 (2018), 193–223; preprint version: Max-Planck-Institut für Mathematik Preprint Series 2014 (26), http://www.mpim-bonn.mpg.de/preblob/5515. MR3769989