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Source. Published p. 221, Theorem 3.3; full proof in Section 4, pp. 232–234. (canonical PDF).

Every finite simplex XX is hyper-Ramsey. Precisely, for every α>0\alpha>0 there are c>1c>1, 0<ϵ<10<\epsilon<1 and an integer m0m_0 such that each m≥m0m\ge m_0 has a finite nonempty witness

Hm⊆S(ρ(X)2+α,m),∣Hm∣<cm,H_m\subseteq S(\sqrt{\rho(X)^2+\alpha},m),\qquad |H_m|<c^m,

and every K⊆HmK\subseteq H_m with ∣K∣≥(1−ϵ)m∣Hm∣|K|\ge(1-\epsilon)^m|H_m| contains a congruent copy of XX. All essential same-paper deductions are proved in the linked pages. The exact deep external inputs remain those stated in Theorem 2.2, Lemma 2.3, and Theorem 3.2.

Proof.

Singletons were handled in definitions. Otherwise, let X={x1,…,xn}X=\{x_1,\ldots,x_n\}, n=d+1≥2n=d+1\ge2. Scaling and radius enlargement reduce the problem to ρ(X)=1\rho(X)=1 and an arbitrary squared slack 0<α<10<\alpha<1: after proving that range, a larger slack follows by lifting, and scaling back multiplies squared slack by ρ(X)2\rho(X)^2.

Let eij=∥xi−xj∥2e_{ij}=\|x_i-x_j\|^2. The negative-type criterion and compactness of the unit zero-sum subspace give γ>0\gamma>0 such that

Qe(λ)≤−γif ∑iλi=0,∑iλi2=1.Q_e(\lambda)\le-\gamma \quad\text{if }\sum_i\lambda_i=0,\quad\sum_i\lambda_i^2=1.

Choose a positive number β\beta with

β<min⁡{γn2,α2n2},\beta<\min\left\{\frac{\gamma}{n^2},\frac{\alpha}{2n^2}\right\},

and define a new zero-diagonal array by eij′=eij−βe'_{ij}=e_{ij}-\beta only for i≠ji\ne j. For every such unit zero-sum vector,

Qe′(λ)=Qe(λ)+β2<0.Q_{e'}(\lambda)=Q_e(\lambda)+\frac\beta2<0.

Theorem 2.1 therefore realizes e′e' as the squared distances of a simplex Z={z1,…,zn}Z=\{z_1,\ldots,z_n\}. In particular, its distinct pair distances are positive; this is a conclusion of the realization criterion. As β↓0\beta\downarrow0, circumradius_continuity gives ρ(Z)→1\rho(Z)\to1. Decrease β\beta further, if needed, so that

ρ(Z)≤1+α/8.\rho(Z)\le1+\alpha/8.

All preceding strict bounds persist under this decrease.

Set μ=1/(n2n)\mu=1/(n2^n) and θ=min⁡{α,βμ}>0\theta=\min\{\alpha,\beta\mu\}>0. Lemma 3.9 produces a simplex V={v1,…,vn}V=\{v_1,\ldots,v_n\} satisfying

∣∥vi−vj∥2−(eij−β)∣≤θ(i≠j),\bigl|\|v_i-v_j\|^2-(e_{ij}-\beta)\bigr|\le\theta\quad(i\ne j),

which is αV\alpha_V-hyper-Ramsey for

αV=ρ(Z)2(1+θ/8)−ρ(V)2>0.\alpha_V=\rho(Z)^2(1+\theta/8)-\rho(V)^2>0.

Define the residual array ff by fii=0f_{ii}=0 and fij=eij−∥vi−vj∥2f_{ij}=e_{ij}-\|v_i-v_j\|^2 for i≠ji\ne j. It satisfies

β(1−μ)≤β−θ≤fij≤β+θ≤β(1+μ)(i≠j).\beta(1-\mu)\le\beta-\theta\le f_{ij} \le\beta+\theta\le\beta(1+\mu)\quad(i\ne j).

These inequalities alone are not being used as an unproved Euclidean realization assertion. The array form of lemma_3_12 constructs a simplex T={t1,…,tn}T=\{t_1,\ldots,t_n\} with precisely these squared distances. Lemma 3.13 then gives its strictly positive admissible squared slack

αT=βn2−ρ(T)2>0.\alpha_T=\beta n^2-\rho(T)^2>0.

By Lemma 3.4, V∗TV*T has density witnesses in every sufficiently large dimension on the sphere whose squared radius is

R02=ρ(V)2+αV+ρ(T)2+αT=ρ(Z)2(1+θ/8)+βn2<(1+α/8)3+α/2≤1+α.\begin{aligned} R_0^2 &=\rho(V)^2+\alpha_V+\rho(T)^2+\alpha_T\\ &=\rho(Z)^2(1+\theta/8)+\beta n^2\\ &<(1+\alpha/8)^3+\alpha/2\le1+\alpha. \end{aligned}

For the last elementary estimate, 0<α<10<\alpha<1 gives

(1+α/8)3−1=3α8+3α264+α3512≤217512α<α2.(1+\alpha/8)^3-1 =\frac{3\alpha}{8}+\frac{3\alpha^2}{64}+\frac{\alpha^3}{512} \le\frac{217}{512}\alpha<\frac\alpha2.

The diagonal subset {(vi,ti):1≤i≤n}\{(v_i,t_i):1\le i\le n\} of V∗TV*T is congruent to XX, because each squared pair distance is

∥vi−vj∥2+∥ti−tj∥2=eij.\|v_i-v_j\|^2+\|t_i-t_j\|^2=e_{ij}.

Consequently those product witnesses force XX at their actual radius R0R_0. Lift them by one constant coordinate to radius 1+α\sqrt{1+\alpha}. As proved in definitions, this preserves all distances and the cardinality estimate and changes the exponential density parameter by at most a fixed factor. With the new dimension m=N+1m=N+1, all sufficiently large integers mm occur. Thus they are the required α\alpha-hyper-Ramsey witnesses for XX. Since the positive squared slack was arbitrary after scaling and lifting, the theorem follows.

Source precision.

The source's Section 4 has the same contraction, approximation, near-regular residual and product-diagonal strategy. The corrected On(β)O_n(\beta) radius budget from Lemma 3.13 requires β<α/(2n2)\beta<\alpha/(2n^2) instead of the printed β<α/(2n2)\beta<\sqrt{\alpha/(2n^2)}. The smaller choice is compatible with all the other requirements and completes the method.

Off-diagonal contraction leaves the diagonal zero. The auxiliary regular simplex in Remark 4.1 has edge length β\sqrt\beta, since β\beta is a squared distance. The existence of the residual simplex, continuity of its predecessor's circumradius, and the final dimension/exponent change are supplied explicitly above. The proof controls the actual containing sphere for the product before passing to its diagonal subset; it does not assume hyper-Ramsey inheritance at an arbitrary smaller intrinsic radius. These are compilation repairs and expansions, not an author-issued erratum.

Dependencies. theorem_2_1, lemma_3_4, lemma_3_9, lemma_3_12, lemma_3_13 and circumradius_continuity.

Bears on. #174.