“…Let us begin with the invariant theory for PSL (2,13). Recall that the six-dimensional representation (the Weil representation) of the finite simple group PSL (2,13) of order 1092, which acts on the five-dimensional projective space P 5 = {(z 1 , z 2 , z 3 , z 4 , z 5 , z 6 ) : z i ∈ C (i = 1, 2, 3, 4, 5, 6)}. This representation is defined over the cyclotomic field Q(e 2πi 13 ).…”