EXACT CLAIM Let p and l be distinct odd primes satisfying p≡2 (mod 3), l≡7 (mod 24), and (p/l)=-1, where the parentheses denote the Legendre symbol. For every a,b≥1, set q=p^a l^b. There are no integers n≥1 and K>1 and no rank-K orthogonal projector P on (C^q)^{⊗n} satisfying both equations (1) and (3) in the problem, for the literal cyclic Weyl errors of weight at most two. In particular this excludes every q=5^a7^b and every q=17^a7^b. No stabilizer or prime-power assumption on K is made. As an ingredient, for any integer q≥2, equations (1) and (3) force the degree-two polynomial L₂(x)=Σ_{j=0}²[z^j](1+(q²−1)z)^{n−x}(1−z)^x to have two distinct integer roots in [5,n]. This is a partial nonexistence theorem, not a solution for all non-prime-power local dimensions. FULL FROZEN PROOF 1. An alphabet-independent quantum Lloyd argument. Write D=q^n, Q=q², and W_g for the tensor-product cyclic Weyl operators, indexed by g in (Z/qZ)^{2n}. These form an orthogonal operator basis: tr(W_g†W_h)=Dδ_{g,h}. Every nonidentity Weyl operator of weight at most four is, up to phase, E†F for distinct errors E,F of weight at most two: partition its nonidentity sites into two sets of size at most two, and choose the local inverse operators on the first set. Thus purity implies PW_gP=0 at weights 1 through 4. Consequently tr(W_g†P)=0 at these weights, since tr(W_g†P)=tr(PW_g†P). Define T_j(A)=Σ_{wt(g)=j}W_g A W_g†. Conjugation acts diagonally on the Weyl basis. At a single site the sum of its conjugation characters over all q² labels is q² for the identity label and zero for every nonidentity label. This holds for composite q as well: each sum factors into geometric sums of powers of the primitive qth root of unity, and a nonzero label gives at least one vanishing sum. After deleting the identity conjugator, the corresponding sums are Q−1 and −1. Therefore, for wt(h)=w, T_j(W_h)=K_j(w)W_h, where K_j(w)=[z^j](1+(Q−1)z)^{n−w}(1−z)^w. The subspaces E(C), for wt(E)≤2, are mutually orthogonal by (1), and perfection says their dimensions sum to D. Hence Σ_{j=0}²T_j(P)=I. Expanding P in the Weyl basis shows that every nonidentity weight w appearing with a nonzero coefficient in P satisfies L₂(w)=0. Such weights are at least five by purity. There must be at least two distinct such weights. Indeed, n=1 is impossible because perfection would give Kq²=q. Thus n≥2, and a weight-two Weyl operator F exists. Suppose that the nonidentity support weights of P comprise at most one value. Choose a polynomial β of degree at most one with β(0)=D/K and vanishing on that support. If the support is empty, choose β constant. As K₀(x)=1 and K₁(x)=(Q−1)n−Qx span the polynomials of degree at most one, write β=β₀K₀+β₁K₁. The diagonalization just proved yields β₀T₀(P)+β₁T₁(P)=I. Right-multiply by FP. Every summand on the left is a multiple of EP E†FP with wt(E)≤1. Here E†F is a nonidentity Weyl operator up to phase and has weight at most three. Purity makes each such summand zero. The right side FP is nonzero, a contradiction. Since L₂ is quadratic with leading coefficient Q²/2, its roots are therefore two distinct integers r,s with 5≤r