Answer

For sufficiency, yes. For necessity, no. This is the part of QUESTION-120 that its readings on the first two uses settle, split off on 2026-10-21 (ADR-049).

  • Sufficiency for distances. THEORY-397 (Active). A random linear map into k ≥ 4(ε²/2 − ε³/3)⁻¹ ln n dimensions keeps every pairwise squared distance within 1 ± ε. Each difference vector’s squared length concentrates, and a union bound over the pairs costs ln n. The proofs cover a random subspace, Gaussian entries and zero-mean ±1 or √3·{+1, 0, −1} entries.
  • Sufficiency for sparse recovery. THEORY-390 (Active). The only assumption is the same per-vector tail. A union bound over (12/δ)^k net points on each of the (eN/k)^k supports, and a step from the net to the whole support, give the restricted isometry property for k ≤ c₁n/log(N/k). Any distribution that yields JL embeddings yields RIP matrices.
  • Necessity for distances. THEORY-395 (Active) shows that some n-point set needs Ω(ε⁻² lg(ε²n)) dimensions under any map, by an encoding argument that counts the supports of k-sparse vectors. THEORY-399 (Active) carries the bound to every ε ≥ 2/√n by counting the bits of a distance sketch. Neither is a tail bound on a random map, and neither could be: they bound every map.
  • Necessity for sparse recovery. THEORY-390 records that the paper takes it from Garnaev–Gluskin’s Gelfand widths of the ℓ₁ ball, which is geometry, not concentration. THEORY-391 (Active) gives the sharp location of ℓ₁ recovery as a limit from counting faces of projected polytopes. A union bound gives only its order.

So the two sufficiency proofs are one argument over two families. Both thresholds are the log of the family’s size over a squared tolerance, and recovery’s family adds a k log(12/δ) term. The necessity proofs are different arguments from that one and from each other. THEORY-395’s count ends at m = Ω(k lg(d/k)), the form of the recovery bound, but that is a reader’s observation in NOTE-925, not a shared proof.

What it leaves to QUESTION-120

The answer covers distances and sparse recovery for random matrices. Whether the superposition toy model is limited by recovery or by incoherence, and whether its phase changes are the Donoho–Tanner transition, stay with the parent. So do random features, whose threshold counts features against samples, and expand-and-threshold maps, which go up in dimension. Whether log(2 + ε²n)/ε² dimensions suffice for one set, as THEORY-393 shows for two, is also open.