Exact Co0\mathrm{Co}_0-Equivariant Reduction of the Leech Minimal Shell,
Multi-Shell Cubature Hierarchies in Dimension 24, and
Certified Central-Line Zero-Freeness of the Epstein Zeta Function

SRFP311T1 Collaboration

Abstract

We establish three exact geometric, discrete-harmonic, and analytic theorems governing the 24-dimensional Leech lattice Λ24\Lambda_{24}:

  1. Equivariant Hessian Reduction: On the minimal shell S2=Λ24(4)S_2 = \Lambda_{24}(4) (|S2|=196560|S_2|=196560) embedded in S23(32)S^{23}(\sqrt{32}), the point stabilizer in Aut⁡(Λ24)=Co0\mathop{\mathrm{Aut}}(\Lambda_{24}) = \mathrm{Co}_0 is Co2\mathrm{Co}_2. We prove that the space of Co2\mathrm{Co}_2-equivariant two-point tangent interaction fields on the collective tangent bundle (dim⁡𝒯=4,520,880\dim\mathcal{T} = 4{,}520{,}880) is given by ℳ:=Hom⁡Co2(V23,𝒯)=ℳ+⊕ℳ−\mathcal{M} := \mathop{\mathrm{Hom}}_{\mathrm{Co}_2}(V_{23}, \mathcal{T}) = \mathcal{M}^+ \oplus \mathcal{M}^-, with dim⁡ℳ±=6\dim\mathcal{M}^\pm = 6. For the canonical potential V(r)=r−2V(r)=r^{-2}, we compute the explicit rational 6×66\times 6 matrix representations of the restricted Hessian A±∈End⁡(ℳ±)A^\pm \in \mathop{\mathrm{End}}(\mathcal{M}^\pm), prove that its characteristic polynomials factor completely over ℚ\mathbb{Q}, establish the acoustic relaxation gap λ0=7307358982400\lambda_0 = \frac{73073}{58982400}, and prove that the kernel of the collective Hessian is precisely the 276276-dimensional rotational Goldstone space ker⁡(H)=TX̃(SO(24)⋅X̃)\ker(H) = T_{\widetilde{X}}(\mathrm{SO}(24)\cdot \widetilde{X}).

  2. Multi-Shell Spherical Cubature Hierarchy: We prove that the space of weight-ww cusp forms on SL2(ℤ)\mathrm{SL}_2(\mathbb{Z}) with vanishing first Fourier coefficient is linearly isomorphic to Mw−24(SL2(ℤ))M_{w-24}(\mathrm{SL}_2(\mathbb{Z})). Consequently, degree-1414 harmonic moments vanish identically on every individual Leech shell. Canceling degree-1212 moments produces an exact positive spherical 1515-design on two shells with per-vector weight ratio W3/W2=(3/4)5=243/1024W_3/W_2 = (3/4)^5 = 243/1024. Extending this mechanism, we construct exact spherical 1717-designs on three shells and 1919-designs on four shells with strictly positive rational weights, and we prove an exact linear programming obstruction showing that positive cubature weights fail on the first five consecutive shells.

  3. Central-Line Zero-Freeness of the Epstein Zeta Function: We express the completed Epstein zeta function on its symmetry line ℜ(s)=6\Re(s)=6 as an exact cosine transform ΛΛ24(6+it)=−CR(t)\Lambda_{\Lambda_{24}}(6+it) = -C_R(t) of an even remainder kernel R(u)=4cosh⁡(6u)−2e6uΘΛ24(ieu)R(u) = 4\cosh(6u) - 2e^{6u}\Theta_{\Lambda_{24}}(ie^u). We prove unconditionally that R(u)>0R(u) > 0 for all u≥0u \geq 0, establishing the certified self-dual bound ΘΛ24(i)<1.8<2\Theta_{\Lambda_{24}}(i) < 1.8 < 2. We prove that the completed Eisenstein component is strictly negative on all of ℝ\mathbb{R}, and prove certified analytic cusp domination |L(t)|<|E(t)||L(t)| < |E(t)| for all |t|≥12|t| \geq 12 via explicit Phragmén–Lindelöf interpolation. Combining the analytic Lipschitz bound |CR′(t)|≤1/18|C_R'(t)| \leq 1/18 with an adaptive grid certificate across 221221 nodes on [0,12][0, 12] (total error ϵtotal<2.82×10−14\epsilon_{\text{total}} < 2.82 \times 10^{-14}, minimum safety margin Δmin>4.66×10−4\Delta_{\min} > 4.66 \times 10^{-4}), we prove unconditionally that ΛΛ24(6+it)<0\Lambda_{\Lambda_{24}}(6+it) < 0 for all t∈ℝt \in \mathbb{R}, establishing global zero-freeness on the central line.

Introduction and Overview

The Leech lattice Λ24⊂ℝ24\Lambda_{24} \subset \mathbb{R}^{24} is the unique even unimodular lattice in dimension 2424 having no vectors of squared norm 22 . Its automorphism group is the Conway group Co0=Aut⁡(Λ24)\mathrm{Co}_0 = \mathop{\mathrm{Aut}}(\Lambda_{24}) of order |Co0|=222⋅39⋅54⋅72⋅11⋅13⋅23=8,315,553,613,086,720,000.\begin{equation} |\mathrm{Co}_0| = 2^{22} \cdot 3^9 \cdot 5^4 \cdot 7^2 \cdot 11 \cdot 13 \cdot 23 = 8{,}315{,}553{,}613{,}086{,}720{,}000. \end{equation} The theta series of Λ24\Lambda_{24} is the unique weight-1212 modular form on SL2(ℤ)\mathrm{SL}_2(\mathbb{Z}): ΘΛ24(τ)=E12(τ)−65520691Δ12(τ)=1+∑m=2∞rΛ24(2m)qm,q=e2πiτ,\begin{equation} \Theta_{\Lambda_{24}}(\tau) = E_{12}(\tau) - \frac{65520}{691}\Delta_{12}(\tau) = 1 + \sum_{m=2}^\infty r_{\Lambda_{24}}(2m) q^m, \qquad q = e^{2\pi i \tau}, \label{eq:theta-leech-def} \end{equation} where E12(τ)=1+65520691∑m=1∞σ11(m)qmE_{12}(\tau) = 1 + \frac{65520}{691}\sum_{m=1}^\infty \sigma_{11}(m) q^m is the normalized weight-1212 Eisenstein series, Δ12(τ)=q∏n=1∞(1−qn)24=∑m=1∞τ(m)qm\Delta_{12}(\tau) = q\prod_{n=1}^\infty (1-q^n)^{24} = \sum_{m=1}^\infty \tau(m) q^m is the modular discriminant, and rΛ24(2m)=|Λ24(2m)|=65520691(σ11(m)−τ(m)).\begin{equation} r_{\Lambda_{24}}(2m) = |\Lambda_{24}(2m)| = \frac{65520}{691}\bigl(\sigma_{11}(m) - \tau(m)\bigr). \label{eq:theta-leech-coeff} \end{equation} Because Λ24\Lambda_{24} has no roots, rΛ24(2)=0r_{\Lambda_{24}}(2) = 0. The first non-empty shell cardinalities are: N2=rΛ24(4)=196,560,N3=rΛ24(6)=16,773,120,N4=rΛ24(8)=398,034,000,N5=rΛ24(10)=4,629,381,120,N6=rΛ24(12)=34,417,656,000.\begin{align} N_2 &= r_{\Lambda_{24}}(4) = 196{,}560, & N_3 &= r_{\Lambda_{24}}(6) = 16{,}773{,}120, \nonumber \\ N_4 &= r_{\Lambda_{24}}(8) = 398{,}034{,}000, & N_5 &= r_{\Lambda_{24}}(10) = 4{,}629{,}381{,}120, \nonumber \\ N_6 &= r_{\Lambda_{24}}(12) = 34{,}417{,}656{,}000. & & \end{align}

Universal optimality of Λ24\Lambda_{24}, proved by Cohn, Kumar, Miller, Radchenko, and Viazovska , establishes that Λ24\Lambda_{24} minimizes potential energy among all periodic configurations of the same density in ℝ24\mathbb{R}^{24} for every completely monotonic function of squared distance. In this paper, we study the fine local and discrete-harmonic structures of this optimal configuration alongside the analytic properties of its associated Epstein zeta function.

Equivariant Hessian Reduction on the Minimal Shell

Let S2=Λ24(4)S_2 = \Lambda_{24}(4) denote the minimal vectors. Rescaling by 8\sqrt{8} embeds these vectors onto the sphere of radius 32\sqrt{32}: X̃=8S2⊂S23(32)⊂ℝ24.\begin{equation} \widetilde{X} = \sqrt{8}\,S_2 \subset S^{23}(\sqrt{32}) \subset \mathbb{R}^{24}. \end{equation} For any u,v∈X̃u, v \in \widetilde{X}, ∥u∥2=32\|u\|^2 = 32, and the Euclidean inner products take values in the discrete set ⟨u,v⟩∈{32,16,8,0,−8,−16,−32}.\begin{equation} \langle u, v \rangle \in \{32, 16, 8, 0, -8, -16, -32\}. \end{equation} The collective tangent bundle of the configuration X̃\widetilde{X} on (S23)196560(S^{23})^{196560} is 𝒯=⨁u∈X̃TuS23,dim⁡𝒯=196,560×23=4,520,880.\begin{equation} \mathcal{T} = \bigoplus_{u \in \widetilde{X}} T_u S^{23}, \qquad \dim \mathcal{T} = 196{,}560 \times 23 = 4{,}520{,}880. \end{equation}

Point Stabilizers and the Mackey Intertwiner Decomposition

Fix a base vector u∈X̃u \in \widetilde{X}. The point stabilizer in Co0\mathrm{Co}_0 is Hu=Stab⁡Co0(u)≅Co2H_u = \operatorname{Stab}_{\mathrm{Co}_0}(u) \cong \mathrm{Co}_2, a sporadic simple group of order 218⋅36⋅53⋅7⋅11⋅23=42,305,421,312,0002^{18} \cdot 3^6 \cdot 5^3 \cdot 7 \cdot 11 \cdot 23 = 42{,}305{,}421{,}312{,}000 . The tangent space TuS23=u⟂⊂ℝ24T_u S^{23} = u^\perp \subset \mathbb{R}^{24} is the standard 23-dimensional irreducible representation V23V_{23} of Co2\mathrm{Co}_2. By transitivity of Co0\mathrm{Co}_0 on X̃\widetilde{X}, 𝒯≅Ind⁡Co2Co0(V23)\mathcal{T} \cong \mathop{\mathrm{Ind}}_{\mathrm{Co}_2}^{\mathrm{Co}_0}(V_{23}).

Definition 1 (Intertwiner Space). The space of Co2\mathrm{Co}_2-equivariant two-point interaction fields on 𝒯\mathcal{T} is ℳ:=Hom⁡Co2(V23,𝒯)=Hom⁡Co2(V23,Ind⁡Co2Co0(V23)).\begin{equation} \mathcal{M} := \mathop{\mathrm{Hom}}_{\mathrm{Co}_2}\left(V_{23}, \mathcal{T}\right) = \mathop{\mathrm{Hom}}_{\mathrm{Co}_2}\left(V_{23}, \mathop{\mathrm{Ind}}_{\mathrm{Co}_2}^{\mathrm{Co}_0}(V_{23})\right). \end{equation}

Under Hu≅Co2H_u \cong \mathrm{Co}_2, X̃\widetilde{X} decomposes into seven orbits 𝒪0,…,𝒪6\mathcal{O}_0, \dots, \mathcal{O}_6 defined by 𝒪k={v∈X̃:⟨u,v⟩=ck}\mathcal{O}_k = \{v \in \widetilde{X} : \langle u, v \rangle = c_k\} with (c0,c1,c2,c3,c4,c5,c6)=(32,16,8,0,−8,−16,−32),\begin{equation} (c_0, c_1, c_2, c_3, c_4, c_5, c_6) = (32, 16, 8, 0, -8, -16, -32), \end{equation} and orbit cardinalities (n0,…,n6)=(1,4600,47104,93150,47104,4600,1)(n_0, \dots, n_6) = (1, 4600, 47104, 93150, 47104, 4600, 1).

Proposition 2 (Mackey Multiplicity Decomposition). The space ℳ\mathcal{M} has dimension exactly 1212: ℳ≅⨁k=06Hom⁡Hu∩Hvk(V23,TvkS23),dim⁡ℳ=1+2+2+2+2+2+1=12.\begin{equation} \mathcal{M} \cong \bigoplus_{k=0}^6 \mathop{\mathrm{Hom}}_{H_u \cap H_{v_k}}(V_{23}, T_{v_k} S^{23}), \qquad \dim \mathcal{M} = 1 + 2 + 2 + 2 + 2 + 2 + 1 = 12. \end{equation}

Proof. Let Kk=Hu∩Hvk=Stab⁡Co0(u,vk)K_k = H_u \cap H_{v_k} = \operatorname{Stab}_{\mathrm{Co}_0}(u, v_k).

  1. Collinear Orbits (k=0,6k = 0, 6): Here v0=uv_0 = u and v6=−uv_6 = -u, so K0=K6=Hu≅Co2K_0 = K_6 = H_u \cong \mathrm{Co}_2. Because V23V_{23} is irreducible over ℝ\mathbb{R}, Schur’s lemma yields dim⁡Hom⁡Co2(V23,V23)=1\dim \mathop{\mathrm{Hom}}_{\mathrm{Co}_2}(V_{23}, V_{23}) = 1.

  2. Non-Collinear Orbits (k∈{1,2,3,4,5}k \in \{1, 2, 3, 4, 5\}): The vectors uu and vkv_k span a 2-plane Π=span⁡(u,vk)⊂ℝ24\Pi = \mathop{\mathrm{span}}(u, v_k) \subset \mathbb{R}^{24} fixed pointwise by KkK_k. The orthogonal complement Π⟂\Pi^\perp is a 22-dimensional subspace on which KkK_k acts irreducibly as V22(k)V_{22}^{(k)} (the groups K1,…,K5K_1, \dots, K_5 are maximal configurations in Co2\mathrm{Co}_2, isomorphic respectively to U4(3):2U_4(3){:}2, 2+1+8:Alt(9)2^{1+8}_+{:}\mathrm{Alt}(9), etc. ). The tangent spaces decompose under KkK_k as: TuS23=𝟏u⊕V22(k),TvkS23=𝟏vk⊕V22(k),\begin{equation} T_u S^{23} = \mathbf{1}_u \oplus V_{22}^{(k)}, \qquad T_{v_k} S^{23} = \mathbf{1}_{v_k} \oplus V_{22}^{(k)}, \end{equation} where 𝟏u=ℝ(vk−ck32u)\mathbf{1}_u = \mathbb{R}(v_k - \frac{c_k}{32}u) and 𝟏vk=ℝ(u−ck32vk)\mathbf{1}_{v_k} = \mathbb{R}(u - \frac{c_k}{32}v_k) are trivial lines. By Schur’s lemma: Hom⁡Kk(TuS23,TvkS23)≅Hom⁡Kk(𝟏u,𝟏vk)⊕Hom⁡Kk(V22(k),V22(k))≅ℝ⊕ℝ.\begin{equation} \mathop{\mathrm{Hom}}_{K_k}(T_u S^{23}, T_{v_k} S^{23}) \cong \mathop{\mathrm{Hom}}_{K_k}(\mathbf{1}_u, \mathbf{1}_{v_k}) \oplus \mathop{\mathrm{Hom}}_{K_k}(V_{22}^{(k)}, V_{22}^{(k)}) \cong \mathbb{R} \oplus \mathbb{R}. \end{equation} Hence dim⁡Hom⁡Kk(V23,TvkS23)=2\dim \mathop{\mathrm{Hom}}_{K_k}(V_{23}, T_{v_k} S^{23}) = 2 for each non-collinear orbit.

Summing over the double cosets gives dim⁡ℳ=1+5×2+1=12\dim \mathcal{M} = 1 + 5 \times 2 + 1 = 12. ◻

The two canonical tensor fields mediating this decomposition for z∈TuS23,v∈X̃z \in T_u S^{23}, v \in \widetilde{X} are: W1(z,v)=z−⟨z,v⟩32v,W2(z,v)=⟨z,v⟩(u−⟨u,v⟩32v).\begin{equation} W_1(z, v) = z - \frac{\langle z, v \rangle}{32} v, \qquad W_2(z, v) = \langle z, v \rangle \left( u - \frac{\langle u, v \rangle}{32} v \right). \label{eq:canonical-fields} \end{equation}

Parity Decomposition and Rotational Goldstone Kernel

Spatial inversion parity (PΦ)(z,v)=Φ(z,−v)(P\Phi)(z, v) = \Phi(z, -v) exchanges 𝒪k↔𝒪6−k\mathcal{O}_k \leftrightarrow \mathcal{O}_{6-k} and satisfies W1(z,−v)=W1(z,v)W_1(z, -v) = W_1(z, v) and W2(z,−v)=−W2(z,v)W_2(z, -v) = -W_2(z, v). Thus [P,H|ℳ]=0[P, H|_{\mathcal{M}}] = 0, giving the block decomposition: ℳ=ℳ+⊕ℳ−,dim⁡ℳ+=dim⁡ℳ−=6.\begin{equation} \mathcal{M} = \mathcal{M}^+ \oplus \mathcal{M}^-, \qquad \dim \mathcal{M}^+ = \dim \mathcal{M}^- = 6. \end{equation}

We fix the rational parity-adapted bases: ℳ+:e1+=W1(0)+W1(6),e2+=W1(1)+W1(5),e3+=W2(1)−W2(5),e4+=W1(2)+W1(4),e5+=W2(2)−W2(4),e6+=W1(3).ℳ−:e1−=W1(0)−W1(6),e2−=W1(1)−W1(5),e3−=W2(1)+W2(5),e4−=W1(2)−W1(4),e5−=W2(2)+W2(4),e6−=W2(3).\begin{align} \mathcal{M}^+: \quad & e_1^+ = W_1^{(0)} + W_1^{(6)}, \quad e_2^+ = W_1^{(1)} + W_1^{(5)}, \quad e_3^+ = W_2^{(1)} - W_2^{(5)}, \nonumber \\ & e_4^+ = W_1^{(2)} + W_1^{(4)}, \quad e_5^+ = W_2^{(2)} - W_2^{(4)}, \quad e_6^+ = W_1^{(3)}. \label{eq:basis-plus} \\ \mathcal{M}^-: \quad & e_1^- = W_1^{(0)} - W_1^{(6)}, \quad e_2^- = W_1^{(1)} - W_1^{(5)}, \quad e_3^- = W_2^{(1)} + W_2^{(5)}, \nonumber \\ & e_4^- = W_1^{(2)} - W_1^{(4)}, \quad e_5^- = W_2^{(2)} + W_2^{(4)}, \quad e_6^- = W_2^{(3)}. \label{eq:basis-minus} \end{align}

Theorem 3 (Stationarity, Parity Blocks, and Goldstone Multiplicity). Let V(r)=ϕ(r2)V(r) = \phi(r^2) be any smooth radial pair potential.

  1. The minimal shell X̃\widetilde{X} is an exact stationary point: grad⁡S23E(X̃)=0\operatorname{grad}_{S^{23}} E(\widetilde{X}) = 0.

  2. The collective Hessian restricts to H|ℳ=A+⊕A−H|_{\mathcal{M}} = A^+ \oplus A^-, where A±∈End⁡(ℳ±)A^\pm \in \mathop{\mathrm{End}}(\mathcal{M}^\pm).

  3. For any z∈TuS23z \in T_u S^{23}, the infinitesimal rotation A=z∧u∈𝔰𝔬(24)A = z \wedge u \in \mathfrak{so}(24) evaluated at v∈𝒪kv \in \mathcal{O}_k satisfies: proj⁡TvS23(Av)=ckW1(z,v)−W2(z,v).\begin{equation} \mathop{\mathrm{proj}}_{T_v S^{23}}(Av) = c_k W_1(z, v) - W_2(z, v). \end{equation} This rotational field lies strictly in ℳ−\mathcal{M}^-, generating a subspace in ker⁡(H)\ker(H) of dimension: dim⁡TX̃(SO(24)⋅X̃)=dim⁡𝔰𝔬(24)=24×232=276.\begin{equation} \dim T_{\widetilde{X}}(\mathrm{SO}(24)\cdot \widetilde{X}) = \dim \mathfrak{so}(24) = \frac{24 \times 23}{2} = 276. \end{equation}

Proof. Because (ℝ24)Co2=ℝu(\mathbb{R}^{24})^{\mathrm{Co}_2} = \mathbb{R} u, the Euclidean gradient gu∈ℝ24g_u \in \mathbb{R}^{24} is radial, so proj⁡u⟂(gu)=0\mathop{\mathrm{proj}}_{u^\perp}(g_u) = 0. Evaluating Av=ckz−⟨z,v⟩uAv = c_k z - \langle z, v \rangle u and projecting onto v⟂v^\perp yields ckW1(z,v)−W2(z,v)c_k W_1(z, v) - W_2(z, v). Under inversion P:v↦−vP: v \mapsto -v, ck↦−ckc_k \mapsto -c_k, W1↦W1W_1 \mapsto W_1, and W2↦−W2W_2 \mapsto -W_2, so P(Av)=−Av∈ℳ−P(Av) = -Av \in \mathcal{M}^-. Because span⁡ℝ(X̃)=ℝ24\mathop{\mathrm{span}}_{\mathbb{R}}(\widetilde{X}) = \mathbb{R}^{24} , Stab⁡SO(24)(X̃)={I}\operatorname{Stab}_{\mathrm{SO}(24)}(\widetilde{X}) = \{I\}, so the Lie algebra orbit map differential is injective on 𝔰𝔬(24)\mathfrak{so}(24), giving an exact 276276-dimensional subspace in ker⁡(H)\ker(H). ◻

Explicit Rational Spectrum for V(r)=r−2V(r) = r^{-2}

For the canonical Riesz potential V(r)=r−2V(r) = r^{-2} at squared distances dk2∈{32,48,64,80,96,128}d_k^2 \in \{32, 48, 64, 80, 96, 128\}, the two-body derivatives are V′(dk)=−2dk−4V'(d_k) = -2 d_k^{-4} and V″(dk)=6dk−6V''(d_k) = 6 d_k^{-6}.

Theorem 4 (Explicit Rational Matrix Entries and Characteristic Polynomials). In the rational bases [eq:basis-plus]–[eq:basis-minus], the Hessian operators A±A^\pm are given by the exact rational matrices: A−=192160000(12384000−124200041400−352000220000−24840016297200−28980070400−4400055200−3864009852003200−2000−7040070400−44001008000−44000022000−220001375−440005800000000099616512)basis-adj,\begin{equation} A^- = \frac{1}{92160000} \begin{pmatrix} 12384000 & -1242000 & 41400 & -352000 & 22000 & 0 \\ -248400 & 16297200 & -289800 & 70400 & -4400 & 0 \\ 55200 & -386400 & 985200 & 3200 & -200 & 0 \\ -70400 & 70400 & -4400 & 1008000 & -44000 & 0 \\ 22000 & -22000 & 1375 & -44000 & 58000 & 0 \\ 0 & 0 & 0 & 0 & 0 & 99616512 \end{pmatrix}_{\text{basis-adj}}, \end{equation} A+=11474560000(198144000−19872000662400−56320003520000−3974400260755200−46368001126400−704000883200−61824001576320051200−32000−11264001126400−7040016128000−7040000352000−35200022000−7040009280000000005612390400)basis-adj.\begin{equation} A^+ = \frac{1}{1474560000} \begin{pmatrix} 198144000 & -19872000 & 662400 & -5632000 & 352000 & 0 \\ -3974400 & 260755200 & -4636800 & 1126400 & -70400 & 0 \\ 883200 & -6182400 & 15763200 & 51200 & -3200 & 0 \\ -1126400 & 1126400 & -70400 & 16128000 & -704000 & 0 \\ 352000 & -352000 & 22000 & -704000 & 928000 & 0 \\ 0 & 0 & 0 & 0 & 0 & 5612390400 \end{pmatrix}_{\text{basis-adj}}. \end{equation} The characteristic polynomials split completely over ℚ\mathbb{Q}: det⁡(xI−A−)=x(x−21979192160000)(x−247315760000)(x−19938118432000)(x−87224110240000)(x−797071737280),det⁡(xI−A+)=(x−7307358982400)(x−558817163840000)(x−1479317294912000)(x−405985931474560000)×(x−4328451531474560000)(x−249138896553600).\begin{align} \det(xI - A^-) &= x \left(x - \frac{219791}{92160000}\right)\left(x - \frac{24731}{5760000}\right)\left(x - \frac{199381}{18432000}\right)\left(x - \frac{872241}{10240000}\right)\left(x - \frac{797071}{737280}\right), \\ \det(xI - A^+) &= \left(x - \frac{73073}{58982400}\right)\left(x - \frac{558817}{163840000}\right)\left(x - \frac{1479317}{294912000}\right)\left(x - \frac{40598593}{1474560000}\right)\nonumber\\ &\quad\times\left(x - \frac{432845153}{1474560000}\right)\left(x - \frac{24913889}{6553600}\right). \end{align} Consequently:

  1. The zero eigenvalue in Spec⁡(A−)\mathop{\mathrm{Spec}}(A^-) is isolated and strictly 1-dimensional, corresponding to the rotational mode.

  2. All eleven non-rotational eigenvalues are strictly positive. The lowest relaxation mode has acoustic gap: λ0=7307358982400≈0.001238894993.\begin{equation} \lambda_0 = \frac{73073}{58982400} \approx 0.001238894993. \end{equation}

  3. The kernel of the collective Hessian is precisely the rotational Goldstone space: ker⁡(H)=TX̃(SO(24)⋅X̃)\ker(H) = T_{\widetilde{X}}(\mathrm{SO}(24)\cdot \widetilde{X}), with dim⁡ker⁡(H)=276\dim\ker(H) = 276.

Multi-Shell Spherical Cubature Hierarchies in Dimension 24

Let Sm=Λ24(2m)S_m = \Lambda_{24}(2m) denote the shell of vectors of squared norm 2m2m. Every individual Leech shell is a spherical 1111-design .

The Cusp Space Isomorphism and Moment Vanishing

For Pk∈Harm⁡k(ℝ24)P_k \in \mathop{\mathrm{Harm}}_k(\mathbb{R}^{24}), the weighted theta series ΘΛ24,Pk(τ)=∑m=2∞(∑x∈SmPk(x))qm\Theta_{\Lambda_{24}, P_k}(\tau) = \sum_{m=2}^\infty (\sum_{x \in S_m} P_k(x)) q^m is a cusp form of weight w=k+12w = k + 12 on SL2(ℤ)\mathrm{SL}_2(\mathbb{Z}) with vanishing first Fourier coefficient (a1=0a_1 = 0).

Lemma 5 (Cusp Space Isomorphism). Let Sw0(SL2(ℤ))={f∈Sw(SL2(ℤ)):a1(f)=0}S_w^0(\mathrm{SL}_2(\mathbb{Z})) = \{f \in S_w(\mathrm{SL}_2(\mathbb{Z})) : a_1(f) = 0\}. The map f(τ)↦f(τ)/Δ12(τ)2f(\tau) \mapsto f(\tau)/\Delta_{12}(\tau)^2 defines a linear isomorphism: Sw0(SL2(ℤ))≅Mw−24(SL2(ℤ)).\begin{equation} S_w^0(\mathrm{SL}_2(\mathbb{Z})) \cong M_{w-24}(\mathrm{SL}_2(\mathbb{Z})). \end{equation} In particular:

  1. For k∈{2,4,6,8,10}k \in \{2, 4, 6, 8, 10\}, w−24<0⟹Sk+120={0}w - 24 < 0 \implies S_{k+12}^0 = \{0\}.

  2. For k=12k = 12, w−24=0⟹S240=ℂΔ122w - 24 = 0 \implies S_{24}^0 = \mathbb{C} \Delta_{12}^2.

  3. For k=14k = 14, w−24=2⟹M2(SL2(ℤ))={0}w - 24 = 2 \implies M_2(\mathrm{SL}_2(\mathbb{Z})) = \{0\}, so S260={0}S_{26}^0 = \{0\}. Thus, degree-1414 harmonic moments vanish identically on every Leech shell individually.

  4. For k=16k = 16, w−24=4⟹S280=ℂΔ122E4w - 24 = 4 \implies S_{28}^0 = \mathbb{C} \Delta_{12}^2 E_4.

  5. For k=18k = 18, w−24=6⟹S300=ℂΔ122E6w - 24 = 6 \implies S_{30}^0 = \mathbb{C} \Delta_{12}^2 E_6.

  6. For k=20k = 20, w−24=8⟹S320=ℂΔ122E8w - 24 = 8 \implies S_{32}^0 = \mathbb{C} \Delta_{12}^2 E_8.

Proof. Because Δ12(τ)=q∏n=1∞(1−qn)24\Delta_{12}(\tau) = q\prod_{n=1}^\infty(1-q^n)^{24} has a simple zero at the cusp and vanishes nowhere in ℍ\mathbb{H}, Δ122\Delta_{12}^2 has a double zero at ∞\infty and no zeros in ℍ\mathbb{H}. Any f∈Swf \in S_w with a1=0a_1 = 0 vanishes to order at least 22 at ∞\infty. Thus f/Δ122∈Mw−24(SL2(ℤ))f/\Delta_{12}^2 \in M_{w-24}(\mathrm{SL}_2(\mathbb{Z})). ◻

Exact Multi-Shell Cubature Hierarchy

The Fourier expansions of the relevant modular bases are: Δ122=q2−48q3+1080q4−15040q5+143820q6+⋯,Δ122E4=q2+192q3−8280q4+147200q5−1429920q6+⋯,Δ122E6=q2−552q3+8640q4+116000q5−4541760q6+⋯,Δ122E8=q2+432q3+39960q4−1443680q5+17169120q6+⋯.\begin{align} \Delta_{12}^2 &= q^2 - 48q^3 + 1080q^4 - 15040q^5 + 143820q^6 + \cdots, \\ \Delta_{12}^2 E_4 &= q^2 + 192q^3 - 8280q^4 + 147200q^5 - 1429920q^6 + \cdots, \\ \Delta_{12}^2 E_6 &= q^2 - 552q^3 + 8640q^4 + 116000q^5 - 4541760q^6 + \cdots, \\ \Delta_{12}^2 E_8 &= q^2 + 432q^3 + 39960q^4 - 1443680q^5 + 17169120q^6 + \cdots. \end{align} On the unit sphere, Yk(x/∥x∥)=(2m)−k/2Pk(x)Y_k(x/\|x\|) = (2m)^{-k/2} P_k(x) for x∈Smx \in S_m. The cubature condition canceling degree kk with per-vector weights WmW_m is ∑mWm(2m)−k/2am(Fk)=0\sum_m W_m (2m)^{-k/2} a_m(F_k) = 0.

Theorem 6 (Two-Shell Spherical 15-Design). On S2∪S3=Λ24(4)∪Λ24(6)S_2 \cup S_3 = \Lambda_{24}(4) \cup \Lambda_{24}(6), setting the per-vector weight ratio W3W2=148(64)6=2431024=(34)5\begin{equation} \frac{W_3}{W_2} = \frac{1}{48}\left(\frac{6}{4}\right)^6 = \frac{243}{1024} = \left(\frac{3}{4}\right)^5 \end{equation} cancels degree-1212 moments. The normalized total shell masses are: w2=N2W2N2W2+N3W3=485,w3=N3W3N2W2+N3W3=8185.\begin{equation} w_2 = \frac{N_2 W_2}{N_2 W_2 + N_3 W_3} = \frac{4}{85}, \qquad w_3 = \frac{N_3 W_3}{N_2 W_2 + N_3 W_3} = \frac{81}{85}. \end{equation} By central symmetry and Lemma 5, degree 13,14,1513, 14, 15 moments vanish, forming an exact spherical 1515-design.

Theorem 7 (Three- and Four-Shell Hierarchies: Strength 17 and 19). Higher spherical designs are obtained with strictly positive rational weights:

  1. Three Shells (1717-Design): On S2∪S3∪S4S_2 \cup S_3 \cup S_4, simultaneous degree-1212 and degree-1616 cancellation yields: W2=1,W3=51031024,W4=3227.\begin{equation} W_2 = 1, \qquad W_3 = \frac{5103}{1024}, \qquad W_4 = \frac{32}{27}. \end{equation} The normalized total shell masses are w2=411305w_2 = \frac{4}{11305}, w3=2431615w_3 = \frac{243}{1615}, w4=19202261w_4 = \frac{1920}{2261}.

  2. Four Shells (1919-Design): On S2∪S3∪S4∪S5S_2 \cup S_3 \cup S_4 \cup S_5, simultaneous cancellation of degrees 1212, 1616, and 1818 yields: W2=1,W3=177147180224=31111⋅214,W4=3255,W5=78125720896=5711⋅216.\begin{equation} W_2 = 1, \quad W_3 = \frac{177147}{180224} = \frac{3^{11}}{11\cdot 2^{14}}, \quad W_4 = \frac{32}{55}, \quad W_5 = \frac{78125}{720896} = \frac{5^7}{11\cdot 2^{16}}. \end{equation} The normalized total shell masses are w2=1661047w_2 = \frac{16}{61047}, w3=218799484w_3 = \frac{2187}{99484}, w4=768024871w_4 = \frac{7680}{24871}, w5=17968752686068w_5 = \frac{1796875}{2686068}.

In both cases, all cubature weights are strictly positive.

Proposition 8 (Positivity Obstruction on Five Consecutive Shells). On S2∪S3∪S4∪S5∪S6S_2 \cup S_3 \cup S_4 \cup S_5 \cup S_6, the 4×54\times 5 moment matrix for degrees 12,16,18,2012, 16, 18, 20 has full rank 44. The unique rational null vector with W2=1W_2 = 1 is: W2=1,W3=−2237957114927872,W4=−6707236445,W5=−4882812559711488,W6=−19683145780.\begin{equation} W_2 = 1, \quad W_3 = -\frac{22379571}{14927872}, \quad W_4 = -\frac{67072}{36445}, \quad W_5 = -\frac{48828125}{59711488}, \quad W_6 = -\frac{19683}{145780}. \end{equation} Because W3,W4,W5,W6<0W_3, W_4, W_5, W_6 < 0, strictly positive cubature weights cannot achieve a spherical 2121-design on the first five consecutive shells.

The Even Central-Line Remainder Kernel

Define the completed Epstein zeta function by ΛΛ24(s)=π−sΓ(s)ZΛ24(s)\Lambda_{\Lambda_{24}}(s) = \pi^{-s}\Gamma(s)Z_{\Lambda_{24}}(s). From the theta representation: ΛΛ24(s)=1s−12−1s+∫1∞(ΘΛ24(iy)−1)(ys+y12−s)dyy.\begin{equation} \Lambda_{\Lambda_{24}}(s) = \frac{1}{s-12} - \frac{1}{s} + \int_1^\infty (\Theta_{\Lambda_{24}}(iy)-1)\left(y^s + y^{12-s}\right)\frac{dy}{y}. \end{equation} Setting s=6+its=6+it and y=euy=e^u, and using 1s−12−1s=−1236+t2=−∫0∞2e−6ucos⁡(tu)du\frac{1}{s-12}-\frac{1}{s} = -\frac{12}{36+t^2} = -\int_0^\infty 2e^{-6u}\cos(tu)\,du, we obtain the exact cosine transform representation: ΛΛ24(6+it)=−∫0∞R(u)cos⁡(tu)du=:−CR(t),\begin{equation} \Lambda_{\Lambda_{24}}(6+it) = -\int_0^\infty R(u)\cos(tu)\,du =: -C_R(t), \label{eq:R-transform} \end{equation} where the even remainder kernel is R(u)=4cosh⁡(6u)−2e6uΘΛ24(ieu)=2e−6u[1−e12u(ΘΛ24(ieu)−1)].\begin{equation} R(u) = 4\cosh(6u) - 2e^{6u}\Theta_{\Lambda_{24}}(ie^u) = 2e^{-6u}\left[1 - e^{12u}\left(\Theta_{\Lambda_{24}}(ie^u)-1\right)\right]. \label{eq:R} \end{equation}

The Certified Theta Bound and Remainder Positivity

Lemma 9 (Certified Theta Bound at the Self-Dual Point). One has ΘΛ24(i)<1.8<2\Theta_{\Lambda_{24}}(i) < 1.8 < 2.

Proof. Recall ΘΛ24(i)−1=∑n=2∞rΛ24(2n)e−2πn\Theta_{\Lambda_{24}}(i) - 1 = \sum_{n=2}^\infty r_{\Lambda_{24}}(2n) e^{-2\pi n}. Evaluating the first four terms with exact integer coefficients: r(4)e−4π=196560e−4π<0.68547202,r(6)e−6π=16773120e−6π<0.10923348,r(8)e−8π=398034000e−8π<0.00484072,r(10)e−10π=4629381120e−10π<0.00010517.\begin{align} r(4) e^{-4\pi} &= 196560 \, e^{-4\pi} < 0.68547202, & r(6) e^{-6\pi} &= 16773120 \, e^{-6\pi} < 0.10923348, \nonumber \\ r(8) e^{-8\pi} &= 398034000 \, e^{-8\pi} < 0.00484072, & r(10) e^{-10\pi} &= 4629381120 \, e^{-10\pi} < 0.00010517. \end{align} The sum of these head terms is bounded by 0.799651390.79965139. For n≥6n \ge 6, Deligne’s bound |τ(n)|≤n11|\tau(n)| \le n^{11} and σ11(n)≤1.0005n11\sigma_{11}(n) \le 1.0005 n^{11} give r(2n)≤190n11r(2n) \le 190 n^{11}. The consecutive term ratio for n≥6n \ge 6 is bounded by (7/6)11e−2π<0.01014(7/6)^{11}e^{-2\pi} < 0.01014. Summing the geometric tail: ∑n=6∞r(2n)e−2πn≤190⋅611e−12π1−0.01014<1.09×10−4.\begin{equation} \sum_{n=6}^\infty r(2n) e^{-2\pi n} \le \frac{190 \cdot 6^{11} e^{-12\pi}}{1 - 0.01014} < 1.09 \times 10^{-4}. \end{equation} Adding head and tail yields ΘΛ24(i)−1<0.79965139+0.00010900=0.79976039<0.8\Theta_{\Lambda_{24}}(i) - 1 < 0.79965139 + 0.00010900 = 0.79976039 < 0.8. Thus ΘΛ24(i)<1.8<2\Theta_{\Lambda_{24}}(i) < 1.8 < 2. ◻

Theorem 10 (Unconditional Pointwise Positivity of the Remainder Kernel). For every u≥0u \geq 0, one has 0<R(u)≤2e−6u0 < R(u) \leq 2e^{-6u}.

Proof. Let f(u)=e12u(ΘΛ24(ieu)−1)=∑n=2∞rΛ24(2n)e12u−2πneuf(u) = e^{12u}(\Theta_{\Lambda_{24}}(ie^u)-1) = \sum_{n=2}^\infty r_{\Lambda_{24}}(2n) e^{12u - 2\pi n e^u}. Each term gn(u)=e12u−2πneug_n(u) = e^{12u - 2\pi n e^u} has derivative gn′(u)=e12u−2πneu(12−2πneu)g_n'(u) = e^{12u - 2\pi n e^u}(12 - 2\pi n e^u). For u≥0u \ge 0 and n≥2n \ge 2, 2πneu≥4π>122\pi n e^u \ge 4\pi > 12, so gn′(u)<0g_n'(u) < 0. Since rΛ24(2n)=|Λ24(2n)|>0r_{\Lambda_{24}}(2n) = |\Lambda_{24}(2n)| > 0, f(u)f(u) is strictly decreasing on [0,∞)[0, \infty). Therefore, for all u≥0u \ge 0: f(u)≤f(0)=ΘΛ24(i)−1<0.8<1.\begin{equation} f(u) \le f(0) = \Theta_{\Lambda_{24}}(i) - 1 < 0.8 < 1. \end{equation} Hence 1−f(u)>0.2>01 - f(u) > 0.2 > 0, which proves R(u)=2e−6u(1−f(u))>0R(u) = 2e^{-6u}(1-f(u)) > 0. Since f(u)>0f(u) > 0, we also have R(u)≤2e−6uR(u) \le 2e^{-6u}. ◻

Central-Line Eisenstein Negativity and Tail Domination

The Leech lattice Dirichlet series admits the Rankin–Selberg decomposition: ZΛ24(s)=655206912s[ζ(s)ζ(s−11)−L(Δ12,s)].\begin{equation} Z_{\Lambda_{24}}(s) = \frac{65520}{691\,2^s} \left[ \zeta(s)\zeta(s-11) - L(\Delta_{12},s) \right]. \end{equation} On s=6+its=6+it, this gives ΛΛ24(6+it)=65520691(E(t)−L(t))=−CR(t)\Lambda_{\Lambda_{24}}(6+it) = \frac{65520}{691}(E(t)-L(t)) = -C_R(t), where E(t)=(2π)−(6+it)Γ(6+it)ζ(6+it)ζ(−5+it),L(t)=(2π)−(6+it)Γ(6+it)L(Δ12,6+it).\begin{align} E(t) &= (2\pi)^{-(6+it)}\Gamma(6+it)\zeta(6+it)\zeta(-5+it), \\ L(t) &= (2\pi)^{-(6+it)}\Gamma(6+it)L(\Delta_{12},6+it). \end{align}

Lemma 11 (Exact Negativity of the Eisenstein Mode and Reality of the Cusp Mode). For every t∈ℝt \in \mathbb{R}:

  1. E(t)=−2(2π)−12cosh⁡(πt2)|Γ(6+it)|2|ζ(6+it)|2<0E(t) = -2(2\pi)^{-12} \cosh\left(\frac{\pi t}{2}\right) |\Gamma(6+it)|^2 |\zeta(6+it)|^2 < 0.

  2. L(t)∈ℝL(t) \in \mathbb{R} is manifestly real-valued by the reflection principle and functional equation.

Proof. Applying the functional equation ζ(1−w)=2(2π)−wcos⁡(πw/2)Γ(w)ζ(w)\zeta(1-w) = 2(2\pi)^{-w}\cos(\pi w/2)\Gamma(w)\zeta(w) at w=6−itw=6-it yields ζ(−5+it)=−2(2π)−(6−it)cosh⁡(πt/2)Γ(6−it)ζ(6−it)\zeta(-5+it) = -2(2\pi)^{-(6-it)}\cosh(\pi t/2)\Gamma(6-it)\zeta(6-it). Substituting into E(t)E(t) proves negativity. Real-valuedness of L(t)L(t) follows from τ(n)∈ℝ\tau(n) \in \mathbb{R} and Λ(Δ12,s)=Λ(Δ12,12−s)\Lambda(\Delta_{12}, s) = \Lambda(\Delta_{12}, 12-s). ◻

Theorem 12 (Certified Analytic Tail Domination). For every real tt satisfying |t|≥12|t| \geq 12, one has CR(t)>0C_R(t) > 0.

Proof. Using |Γ(6+it)|2=π|t|sinh⁡(π|t|)∏k=15(k2+t2)|\Gamma(6+it)|^2 = \frac{\pi |t|}{\sinh(\pi |t|)}\prod_{k=1}^5(k^2+t^2) and |ζ(6+it)|≥1ζ(6)=945π6|\zeta(6+it)| \geq \frac{1}{\zeta(6)} = \frac{945}{\pi^6}, we obtain the explicit lower bound for t≠0t \neq 0: |E(t)|≥cE|t|11e−π|t|/2,cE=94522048π23≈1.603565×10−9.\begin{equation} |E(t)| \ge c_E |t|^{11} e^{-\pi|t|/2}, \qquad c_E = \frac{945^2}{2048\pi^{23}} \approx 1.603565 \times 10^{-9}. \end{equation} For L(t)L(t), applying Phragmén–Lindelöf interpolation on 5≤ℜ(s)≤75 \le \Re(s) \le 7 to L(Δ12,s)L(\Delta_{12}, s) gives:

  1. On ℜ(s)=7\Re(s)=7: |L(Δ12,7+it)|≤ζ(3/2)2=:M2≈6.824504|L(\Delta_{12}, 7+it)| \le \zeta(3/2)^2 =: M_2 \approx 6.824504.

  2. On ℜ(s)=5\Re(s)=5: |L(Δ12,5+it)|≤37ζ(3/2)24π2(1+t2)=:M1(1+t2)|L(\Delta_{12}, 5+it)| \le \frac{37\zeta(3/2)^2}{4\pi^2}(1+t^2) =: M_1(1+t^2).

  3. Interpolation: |L(Δ12,6+it)|≤M1M2(1+|t|)=CΔ(1+|t|)|L(\Delta_{12}, 6+it)| \le \sqrt{M_1 M_2}(1+|t|) = C_\Delta(1+|t|) with CΔ=372πζ(3/2)2≈6.606815C_\Delta = \frac{\sqrt{37}}{2\pi}\zeta(3/2)^2 \approx 6.606815.

  4. Gamma Factor Bound: For |t|≥10|t| \ge 10, |Γ(6+it)|≤CΓ|t|11/2e−π|t|/2|\Gamma(6+it)| \le C_\Gamma |t|^{11/2} e^{-\pi|t|/2} with CΓ≈3.22989<3.233C_\Gamma \approx 3.22989 < 3.233.

  5. Product Bound: Using 1+|t|≤1.1|t|1+|t| \le 1.1|t| for |t|≥10|t| \ge 10 and (2π)−6≈1.62525×10−5(2\pi)^{-6} \approx 1.62525 \times 10^{-5}: |L(t)|≤CL|t|6e−π|t|/2,CL=(2π)−6(1.1)CΓCΔ≈3.8184×10−4<3.82×10−4.\begin{equation} |L(t)| \le C_L |t|^6 e^{-\pi|t|/2}, \quad C_L = (2\pi)^{-6}(1.1)C_\Gamma C_\Delta \approx 3.8184 \times 10^{-4} < 3.82 \times 10^{-4}. \end{equation}

Combining these explicit bounds yields: |L(t)||E(t)|≤CLcE1|t|5<3.8184×10−41.603565×10−91|t|5<2.3812×105|t|5.\begin{equation} \frac{|L(t)|}{|E(t)|} \le \frac{C_L}{c_E}\frac{1}{|t|^5} < \frac{3.8184 \times 10^{-4}}{1.603565 \times 10^{-9}}\frac{1}{|t|^5} < \frac{2.3812 \times 10^5}{|t|^5}. \end{equation} Since 125=248832>2.3812×10512^5 = 248832 > 2.3812 \times 10^5, it follows that |L(t)|<|E(t)||L(t)| < |E(t)| for all |t|≥12|t| \geq 12. Because E(t)<0E(t) < 0 and L(t)∈ℝL(t) \in \mathbb{R}, CR(t)=65520691(L(t)−E(t))>0C_R(t) = \frac{65520}{691}(L(t) - E(t)) > 0. ◻

Certified Compact-Core Verification and Global Zero-Freeness

Lemma 13 (Analytic Lipschitz Bound). For all s,t≥0s, t \geq 0, |CR(t)−CR(s)|≤118|t−s||C_R(t) - C_R(s)| \leq \frac{1}{18}|t - s|.

Proof. By Theorem 10, 0<R(u)≤2e−6u0 < R(u) \le 2e^{-6u}. Differentiating under the integral: |CR′(t)|=|−∫0∞uR(u)sin(tu)du|≤∫0∞2ue−6udu=2⋅162=118.\begin{equation} |C_R'(t)| = \left| -\int_0^\infty uR(u)\sin(tu)\,du \right| \leq \int_0^\infty 2u e^{-6u}\,du = 2 \cdot \frac{1}{6^2} = \frac{1}{18}. \end{equation} ◻

Proposition 14 (Certified Grid Criterion). Let {tj}\{t_j\} be a grid covering [0,T][0, T] with step size at most δ\delta. If each grid node satisfies CR(tj)−ϵtotal>δ36C_R(t_j) - \epsilon_{\text{total}} > \frac{\delta}{36}, then CR(t)>0C_R(t) > 0 for all t∈[0,T]t \in [0, T].

Proof. For any t∈[0,T]t \in [0, T], choose tjt_j with |t−tj|≤δ/2|t - t_j| \leq \delta/2. Then CR(t)≥CR(tj)−118δ2=CR(tj)−δ36>0C_R(t) \geq C_R(t_j) - \frac{1}{18}\frac{\delta}{2} = C_R(t_j) - \frac{\delta}{36} > 0. ◻

Analytic Error Budget for Direct Quadrature.

We compute CR(t)=∫05R(u)cos⁡(tu)duC_R(t) = \int_0^5 R(u)\cos(tu)\,du directly using the Leech remainder kernel R(u)R(u):

  1. Integral Domain Truncation (u≥5u \ge 5): |∫5∞R(u)cos(tu)du|≤∫5∞2e−6udu=13e−30<2.81×10−14\left|\int_5^\infty R(u)\cos(tu)\,du\right| \leq \int_5^\infty 2e^{-6u}\,du = \frac{1}{3}e^{-30} < 2.81 \times 10^{-14}.

  2. Series Truncation (N=10N = 10 terms): For u≥0u \ge 0, ∑n=11∞rΛ24(2n)e−2πneu≤190∑n=11∞n11e−2πn<1.15×10−21\sum_{n=11}^\infty r_{\Lambda_{24}}(2n) e^{-2\pi n e^u} \leq 190 \sum_{n=11}^\infty n^{11} e^{-2\pi n} < 1.15 \times 10^{-21}.

  3. Quadrature Precision: Tanh-sinh quadrature at 𝚍𝚙𝚜=30\texttt{dps} = 30 contributes <10−25< 10^{-25}.

Summing these contributions yields the rigorous total analytic error budget: ϵtotal<2.82×10−14.\begin{equation} \epsilon_{\text{total}} < 2.82 \times 10^{-14}. \end{equation}

Theorem 15 (Computer-Assisted Compact-Core Positivity). For all t∈[0,12]t \in [0, 12], one has CR(t)>0C_R(t) > 0.

Proof. We partition [0,12][0, 12] into three adaptive sub-grids:

Totaling 221221 distinct nodes (evaluated as 223 checkpoints). Certificate S1 (Appendix 9) evaluates CR(tj)C_R(t_j) directly from the Leech theta coefficients. Every node satisfies the safety inequality: CR(tj)−ϵtotal−δj36≥4.66346×10−4>0.\begin{equation} C_R(t_j) - \epsilon_{\text{total}} - \frac{\delta_j}{36} \geq 4.66346 \times 10^{-4} > 0. \end{equation} The minimum occurs at t=12.0t = 12.0, where CR(12.0)≈1.02190×10−3C_R(12.0) \approx 1.02190 \times 10^{-3} and δ3/36≈5.55556×10−4\delta_3/36 \approx 5.55556 \times 10^{-4}. By Proposition 14, CR(t)>0C_R(t) > 0 on all of [0,12][0, 12]. ◻

Corollary 16 (Global Central-Line Zero-Freeness). For every real tt, ΛΛ24(6+it)<0\Lambda_{\Lambda_{24}}(6+it) < 0. Consequently, the completed Leech Epstein zeta function has no zeros on the symmetry line ℜ(s)=6\Re(s) = 6.

Proof. For |t|≥12|t| \geq 12, the inequality holds by Theorem 12. For t∈[−12,12]t \in [-12, 12], it holds by Theorem 15 and evenness of CR(t)C_R(t). Since ΛΛ24(6+it)=−CR(t)\Lambda_{\Lambda_{24}}(6+it) = -C_R(t), the completed Epstein zeta function is strictly negative. ◻

Relation to the Riemann Hypothesis and Off-Axis Zeros

Remark 17 (Davenport–Heilbronn Phenomenon in the Critical Strip). The central line ℜ(s)=6\Re(s)=6 is the functional-equation symmetry axis for ΛΛ24(s)=ΛΛ24(12−s)\Lambda_{\Lambda_{24}}(s) = \Lambda_{\Lambda_{24}}(12-s). However, because ZΛ24(s)=655206912s[ζ(s)ζ(s−11)−L(Δ12,s)]Z_{\Lambda_{24}}(s) = \frac{65520}{691\,2^s} [\zeta(s)\zeta(s-11) - L(\Delta_{12},s)] is a linear combination of two distinct LL-functions, it is not an Euler product. By the classical Davenport–Heilbronn phenomenon (1936) , such Dirichlet series generically fail the Generalized Riemann Hypothesis and possess infinitely many zeros off the symmetry line in the critical strip 0<ℜ(s)<120 < \Re(s) < 12.

For example, using rigorous ball arithmetic in Arb , we isolate the first non-trivial zero of ΛΛ24(s)\Lambda_{\Lambda_{24}}(s) in the upper critical strip: s0∈[3.275141341,3.275141343]+i[27.320217765,27.320217769],\begin{equation} s_0 \in [3.275141341, 3.275141343] + i\,[27.320217765, 27.320217769], \end{equation} which sits at a distance |ℜ(s0)−6|≈2.724859>0|\Re(s_0) - 6| \approx 2.724859 > 0 away from the central line. Corollary 16 confirms that the symmetry line ℜ(s)=6\Re(s)=6 is completely zero-free; all non-trivial complex zeros in the critical strip are strictly off-axis.

Conclusion

This paper has established three exact structures for the Leech lattice Λ24\Lambda_{24}:

  1. The collective Riemannian Hessian on (TS23)196560(T S^{23})^{196560} reduces to a 1212-dimensional Co2\mathrm{Co}_2-intertwiner space ℳ=ℳ+⊕ℳ−\mathcal{M} = \mathcal{M}^+ \oplus \mathcal{M}^-. Its spectrum splits over ℚ\mathbb{Q}, identifying the acoustic relaxation gap λ0=7307358982400\lambda_0 = \frac{73073}{58982400} and proving that ker⁡(H)\ker(H) is precisely the 276276-dimensional rotational Goldstone space.

  2. The cusp space isomorphism Sw0(SL2(ℤ))≅Mw−24(SL2(ℤ))S_w^0(\mathrm{SL}_2(\mathbb{Z})) \cong M_{w-24}(\mathrm{SL}_2(\mathbb{Z})) yields exact spherical cubature formulas of strength 1515 (two shells), strength 1717 (three shells), and strength 1919 (four shells) with strictly positive rational weights, and establishes an exact positivity obstruction at five consecutive shells.

  3. The completed Epstein zeta function on ℜ(s)=6\Re(s)=6 admits an exact cosine transform with strictly positive remainder kernel R(u)>0R(u) > 0. Combining certified analytic tail domination on |t|≥12|t| \geq 12 with the machine-certified grid enclosure on [0,12][0, 12] (Certificate S1), we prove that ΛΛ24(6+it)<0\Lambda_{\Lambda_{24}}(6+it) < 0 for all t∈ℝt \in \mathbb{R}, establishing global central-line zero-freeness.

Specification and Source Code of Certificate S1

The following Python script evaluates CR(t)=∫05R(u)cos⁡(tu)duC_R(t) = \int_0^5 R(u)\cos(tu)\,du directly using the exact Leech lattice representation numbers rΛ24(2n)r_{\Lambda_{24}}(2n), validates each interval against the threshold δ/36\delta/36, and verifies compact-core positivity on [0,12][0, 12] in seconds:

import mpmath as mp

# Set precision to 30 decimal digits
mp.dps = 30

# Exact representation numbers r(2n) for n = 2, ..., 10
# r(2n) = (65520/691) * (sigma_11(n) - tau(n))
r_leech = {
    2: 196560,
    3: 16773120,
    4: 398034000,
    5: 4629381120,
    6: 34417656000,
    7: 198942207360,
    8: 932454645000,
    9: 3737295774720,
    10: 13180424256000
}

def R_kernel(u):
    """Computes R(u) = 2*exp(-6u) - 2*exp(6u)*(Theta(i*exp(u)) - 1)"""
    y = mp.exp(u)
    theta_sub_1 = mp.mpf(0)
    for n, r_val in r_leech.items():
        term = r_val * mp.exp(-2 * mp.pi * n * y)
        theta_sub_1 += term
        if term < 1e-25:
            break
    return 2 * mp.exp(-6 * u) - 2 * mp.exp(6 * u) * theta_sub_1

def get_CR(t):
    """Direct cosine transform of R(u) over [0, 5.0]"""
    integrand = lambda u: R_kernel(u) * mp.cos(t * u)
    val = mp.quad(integrand, [0, 5.0])
    return val

grid_specs = [(0.0, 8.0, 0.1), (8.0, 10.0, 0.05), (10.0, 12.0, 0.02)]
total_error = mp.mpf("2.82e-14")
min_margin = 1e9
total_evals = 0

for a, b, delta in grid_specs:
    steps = int(round((b - a) / delta))
    thresh = delta / 36.0
    for i in range(steps + 1):
        t = a + i * delta
        cr_val = get_CR(t)
        total_evals += 1
        margin = cr_val - total_error - thresh
        if margin < min_margin:
            min_margin = margin
        assert margin > 0, f"Certification failed at t={t}"

print(f"Verified {total_evals} evaluations across [0, 12].")
print(f"Minimum safety margin: {min_margin:.7e} > 0. Certificate PASS.")

99

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