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Source. Published p. 232, Lemma 3.12, where it is quoted from Frankl–Rödl (1990). The finite cut-vector proof below is supplied by the compilation. (canonical PDF).

As printed (p. 232): for every integer d≥1d\ge1 there is a real 1≥μ=μ(d+1)>01\ge\mu=\mu(d+1)>0 such that, for every (μ,β)(\mu,\beta)-regular simplex T={t1,…,td+1}T=\{t_1,\ldots,t_{d+1}\}, there is a (d+12)\binom{d+1}2-dimensional box PP (the vertex set of a rectangular parallelepiped) containing a subset T′T' congruent to TT.

Array form proved here. Let n=d+1≥2n=d+1\ge2, M=(n2)M=\binom n2, and choose

μn=1n2n.\mu_n=\frac1{n2^n}.

For every β>0\beta>0, every symmetric zero-diagonal array ee with

∣eij/β−1∣≤μn(i≠j)|e_{ij}/\beta-1|\le\mu_n\quad(i\ne j)

is realized by an affinely independent set of nn vertices of a box PP with at most MM nonconstant coordinates. The box can be chosen so that

ρ(P)2≤Mβ(1+μn)4≤Mβ2<βn2.\rho(P)^2\le\frac{M\beta(1+\mu_n)}4 \le\frac{M\beta}{2}<\beta n^2.

Thus the source's box dimension can be read as an upper bound, with unused constant coordinates omitted. The array need not be assumed Euclidean in advance.

Proof.

Index the coordinates of RM\mathbb R^M by unordered pairs of [n][n]. For every nonempty proper subset S⊂[n]S\subset[n], let δS\delta_S have coordinate one on pairs separated by SS and zero on other pairs. Also write δ[n]=0\delta_{[n]}=0. Each pair is separated by exactly 2n−12^{n-1} subsets, so

∑∅≠S⊊[n]21−nδS=1.\sum_{\varnothing\ne S\subsetneq[n]}2^{1-n}\delta_S=\mathbf1.

If EijE_{ij} is the unit vector for pair {i,j}\{i,j\}, then

2Eij=δ{i}+δ{j}−δ{i,j}.2E_{ij}=\delta_{\{i\}}+\delta_{\{j\}}-\delta_{\{i,j\}}.

This identity also holds when n=2n=2, since the final cut is zero. Put hij=eij/β−1h_{ij}=e_{ij}/\beta-1. Start with coefficient wS=21−nw_S=2^{1-n} on every nontrivial cut and, for each pair ijij, add hij/2h_{ij}/2 to the two singleton-cut coefficients and subtract hij/2h_{ij}/2 from the {i,j}\{i,j\} coefficient if that cut is nontrivial. Then

∑SwSδS=e/β.\sum_S w_S\delta_S=e/\beta.

For n≥3n\ge3, a singleton coefficient changes in absolute value by at most (n−1)μn/2(n-1)\mu_n/2, a two-element coefficient by at most μn/2\mu_n/2, and other coefficients do not change. For n=2n=2, each singleton changes by at most μn/2\mu_n/2. These bounds are all strictly smaller than 21−n2^{1-n}, so every wSw_S is positive.

If more than MM cuts have positive coefficients, they are linearly dependent in RM\mathbb R^M. Choose a nonzero relation ∑SλSδS=0\sum_S\lambda_S\delta_S=0, with some λS>0\lambda_S>0 after changing its sign if needed, and set

t=min⁡λS>0wSλS,wS′=wS−tλS.t=\min_{\lambda_S>0}\frac{w_S}{\lambda_S},\qquad w'_S=w_S-t\lambda_S.

All new coefficients are nonnegative, at least one is zero, and the represented array is unchanged. Repeating this finite operation leaves at most MM positive coefficients.

For each surviving cut SS, give the box a coordinate edge of length βwS\sqrt{\beta w_S}, and give its ii-th selected vertex that coordinate exactly when i∈Si\in S. The squared distance between vertices i,ji,j is β∑SwSδS(i,j)=eij\beta\sum_Sw_S\delta_S(i,j)=e_{ij}. The points are distinct because eij≥β(1−μn)>0e_{ij}\ge\beta(1-\mu_n)>0.

They are also affinely independent. For a zero-sum vector λ\lambda with ∑iλi2=1\sum_i\lambda_i^2=1,

Qe(λ)=−β2+β∑i<jhijλiλj≤−β2+βμn(n−1)2<0,\begin{aligned} Q_e(\lambda) &=-\frac\beta2+\beta\sum_{i<j}h_{ij}\lambda_i\lambda_j\\ &\le-\frac\beta2+\frac{\beta\mu_n(n-1)}2<0, \end{aligned}

where ∑i<j∣λiλj∣≤(n−1)/2\sum_{i<j}|\lambda_i\lambda_j|\le(n-1)/2 follows from (∑i∣λi∣)2≤n(\sum_i|\lambda_i|)^2\le n. Theorem 2.1 gives affine independence.

Every surviving cut separates at least one pair. Its squared edge length βwS\beta w_S is at most that pair's squared distance and hence at most β(1+μn)\beta(1+\mu_n). A box has squared circumradius one quarter of the sum of its squared edge lengths. There are at most MM of them, proving the radius estimate and the lemma.

Source precision.

The source refers to the 1990 near-regular embedding. Its original incidence proof and padding argument are preserved separately. The proof here supplies the all-nn array realization and stated dimension bound by a different elementary finite argument; it is not an author-issued correction. It avoids assuming a metric realization of a later residual array. Its explicit μn\mu_n is sufficient, not claimed optimal.

Bears on. #174.