“…In the OD theory, a crystal structure is described with (i) a set of partial symmetry operations (POs) transforming a structural block (an OD layer) into itself (k-POs) and (ii) a set of POs transforming an OD layer into an adjacent one above it (r-POs) [13,15,18,21]. In the case of the Mg-TM-RE LPSO/OD phases, a set of k-POs is described with the layer group of P( 3)1m irrespective of the number of close-packed atomic layers (either 5, 6, 7 or 8), as far as an OD layer is selected so that TM 6 RE 8 atomic clusters with the L1 2 -type atomic arrangement are periodically arranged on lattice points of a 2 ffiffiffi 3 p a Mg  2 ffiffiffi 3 p a Mg two-dimensional primitive hexagonal lattice [13,15,18].…”