“…We have two more chiral operators than the allowed monopole states. However, since we already have an imposed relation among those operators, (Tr 1 X) 2 |1, 1, 0, 0 , Tr 1 X 2 |1, 1, 0, 0 , (Tr 1 X) (Tr 2 X) |1, 1, 0, 0 , (Tr 2 X) 2 |1, 1, 0, 0 , Tr 2 X 2 |1, 1, 0, 0 (C. 26) while the allowed chiral operators composed of the lower dimensional monopole operators are (X 1 ) 2 W + 0 , X 2 W + 0 , X 1 V , which span the monopole states (C.26) together with composites of the lower dimensional monopole operators. We emphasize that while we don't specify the exact map between those two operators and the monopole states in (C.26), from the counting, we do know that those two, which carry global charges…”