Enumerate all k-sets as K(i)={u1(i)<⋯<uk(i)},
1≤i≤r. The construction is as follows. Partition [n] into
pairwise disjoint core blocks L1,…,Ls, each of size l, and
blocks Cw, each of size b, for every word w∈{0,…,k}r.
Set
For a unit vector a=(a1,…,ak), put a0=0 and define
vi∈Rn to have coordinate aj/l on Aj(i).
Also set yi=spread(a,K(i)).
These partitions have common part sizes (l0,…,lk); every full
joint cell has size at least b=λn; and the vi are linearly,
hence affinely, independent. For every i=h,
0≤∥vi−vh∥2−∥yi−yh∥2≤lq4(n−ls).
They all have squared norm 1+(n−ls)/(lq). If r=1, the pairwise
assertions are vacuous and the other conclusions remain valid.
The printed lemma (p. 224) assumes only that l,s,k,n are integers with
n>ls and (k+1)(ks) dividing n−ls, and asserts (9) every
joint cell has size at least λn, (10) the vectors are affinely
independent, and (11) the two-sided bound
∣∥vi−vh∥2−∥yi−yh∥2∣≤4(n−ls)/(l(k+1)) for i=h. The
ranges s≥k≥1, l≥1, the common part sizes, linear independence,
the lower bound 0 and the norm formula are made explicit here.
Proof.
The stated blocks exist because their total size is
sl+bqr=n. claim_3_6 proves the common part sizes and positive
joint cells directly from this construction.
Choose an index j with aj=0, which exists since ∥a∥=1.
For each row i, a coordinate in the nonempty block
C(0,…,0,j,0,…,0), with j in position i, is nonzero
in vi and zero in all other vh. Thus any relation
∑iνivi=0 has νi=0 for every i. This proves linear
independence even when some coefficients of a vanish or coincide.
On the core blocks, each coordinate of yi is repeated l times and
divided by l. The core contribution to
∥vi−vh∥2 is therefore exactly ∥yi−yh∥2. For r≥2,
each pair of labels (j,j′)∈{0,…,k}2 occurs in exactly
qr−2 of the added blocks when rows i,h are fixed. Equivalently,
this follows from claim_3_7. Hence
The extra term is nonnegative. Since a0=0 and
∑j=0kaj2=1, the inequality
(aj−aj′)2≤2aj2+2aj′2 bounds the double sum by 4q.
Substitution of bqr=n−ls gives the claimed error.
Finally, each nonzero label part has size l+bqr−1, so
∥vi∥2=j=1∑kll+bqr−1aj2=1+lbqr−1=1+lqn−ls.
This also proves the norm statement in the one-row case.
Source precision.
The positivity and integrality of all parameters, and disjointness
of the added blocks from the core blocks, are explicit here. The full joint
pattern, not only its pairwise marginals, is needed later. The elementary
bound 4q is the source's sufficient bound, not an optimal estimate.