EXACT CLAIM A constructive exclusion for an explicit non-transpose-symmetric PPT-entangled family. Let A=E=C³, let 0. Define p=|00>+|11>+|22>, v=|20>+t|22>, and H_t=s[|p>,|02>,|10>,|12>,|21> are linearly independent, and their coefficients in H_t are strictly positive. Consequently H_t≥0 and rank(H_t)=7. Direct partial trace gives Tr_E H_t=diag(3s,3s,s+2)=M_t. Since s>0, W_t exists and J_t is a positive operator with input marginal I_A, hence is the Choi operator of a channel. PPT and ranks. The partial transpose H_t^Γ is block diagonal in the following orthogonal decomposition. On |00> and |11> its singleton blocks are s. On each ordered pair (|01>,|10>) and (|12>,|21>) its block is s[[1,1],[1,1]]. On (|02>,|20>,|22>) its block is [[s,s,0],[s,1,t],[0,t,1]] = s f f^T + g g^T, where f=(1,1,0)^T and g=(0,t,1)^T. This last identity uses s+t²=1. The last block is positive of rank two because f and g are independent; the other nonsingleton blocks each have rank one. Hence H_t^Γ≥0 and rank(H_t^Γ)=2+1+1+2=6. Invertible congruence by W_t⊗I preserves both ranks and positivity, and commutes with Γ. These assertions therefore hold for J_t. Unitary conjugation preserves rank, proving the stated absence of output-unitary transpose symmetry. Entanglement. Two vectors in ker H_t are |00>−|11> and |00>+t|20>−|22>. Three vectors in ker H_t^Γ are |01>−|10>, |12>−|21>, and |02>−|20>+t|22>. Suppose nonzero x,y satisfy x⊗y∈ran H_t and x⊗conj(y)∈ran H_t^Γ. Orthogonality to these real kernel vectors gives x0 y0=x1 y1, x0 y0+t x2 y0−x2 y2=0, x0 conj(y1)=x1 conj(y0), x1 conj(y2)=x2 conj(y1), x0 conj(y2)−x2 conj(y0)+t x2 conj(y2)=0. If y1≠0, the third and fourth equations imply x=c conj(y), where c=x1/conj(y1). Here c≠0, since otherwise x=0. Substitution into the fifth equation gives tc conj(y2)²=0, so y2=x2=0. The second equation now gives x0 y0=0, and the first then gives x1 y1=0, a contradiction. Thus y1=0. Since y≠0, the third and fourth equations now force x1=0. If H_t were separable, it would be a finite positive sum of product projectors |x⊗y> component. This contradicts <11|H_t|11>=s>0. Hence H_t is entangled. Invertible local filtering preserves separability in both directions, so J_t is entangled as well. Positive symmetric extension. Introduce E'≅C³ and order tensor factors A,E,E'. Set w=|000>+|101>+|110>+|202>+|220>+t|222>, z=|2>⊗(|0>+t|2>)⊗(|0>+t|2>), Ω_t=s[|w><011|+|022><022|+|122><122|+|211><211|]+[t²/(1+t²)]|z>, and v. Thus Tr_{E'}|w><10|+|v>,|02>,|12>,|21>, respectively. Finally, Tr_{E'}|z>