It is however very difficult to combine the SU(2) symmetry with the lattice symmetries in a computationally useful way (non-sparse and computationally expensive matrices)
Note the finer structure of block on SU(N) symmetry. The J conserved block (basis of one irep of SU(N)) can be further decomposed into sub-block of dimension the same as multiplicity instead of the dimension of irep! (This is because Jz conservation U(1) is included in J conservation SU(2))
Useful links on ED
Nauty, a set of very efficient C language procedures for determining the automorphism group of a vertex-colored graph.
relevant papers on ED technique for SU(2) symmetry