“…The tensor T is a composition of cross-sectional measurements that includes in it effects due to both crystal structure [3,4] and experimental aberration [5,6]. In such 3D scattering applications it would be desirable to represent T as a product of matrices, e.g., T = ( n P n )M( m P m ), such that M again describes the scattering, and a P i (for i = n or m) might describe the transport of either a neutron-optical component or aberration imposed by some sample environment fixture [6]. To facilitate this product as a matrix multiplication, the P i need to have the same rank and dimension as the Blume-Maleev tensor.…”