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Input space group symbol: -C 4c
Convention: Hall symbol

Number of lattice translations: 2
Space group is centric.
Number of representative symmetry operations: 4
Total number of symmetry operations: 16

Parallelepiped containing an asymmetric unit:
  cctbx Error: Brick is not available for the given space group representation.

List of symmetry operations:
Matrix Rotation-part type Axis direction Screw/glide component Origin shift
x,y,z 1---
-y,x,z+1/2 4^1[0,0,1]0,0,1/20,0,0
-x,-y,z 2[0,0,1]0,0,00,0,0
y,-x,z+1/2 4^-1[0,0,1]0,0,1/20,0,0
-x,-y,-z -1--0,0,0
y,-x,-z-1/2 -4^1[0,0,1]0,0,00,0,-1/4
x,y,-z -2[0,0,1]0,0,00,0,0
-y,x,-z-1/2 -4^-1[0,0,1]0,0,00,0,-1/4
x+1/2,y+1/2,z 1---
-y+1/2,x+1/2,z+1/2 4^1[0,0,1]0,0,1/20,1/2,0
-x+1/2,-y+1/2,z 2[0,0,1]0,0,01/4,1/4,0
y+1/2,-x+1/2,z+1/2 4^-1[0,0,1]0,0,1/21/2,0,0
-x+1/2,-y+1/2,-z -1--1/4,1/4,0
y+1/2,-x+1/2,-z-1/2 -4^1[0,0,1]0,0,01/2,0,-1/4
x+1/2,y+1/2,-z -2[0,0,1]1/2,1/2,00,0,0
-y+1/2,x+1/2,-z-1/2 -4^-1[0,0,1]0,0,00,1/2,-1/4

Space group number: 84
Conventional Hermann-Mauguin symbol: P 42/m
Universal    Hermann-Mauguin symbol: P 42/m (a+b,-a+b,c)
Hall symbol: -P 4c (1/2*x+1/2*y,-1/2*x+1/2*y,z)
Change-of-basis matrix: x-y,x+y,z
               Inverse: 1/2*x+1/2*y,-1/2*x+1/2*y,z

List of Wyckoff positions:
Wyckoff letter Multiplicity Site symmetry
point group type
Representative special position operator
k161x,y,z
j8mx,y,0
i821/4,1/4,z
h821/2,0,z
g820,0,z
f4-41/2,0,1/4
e4-40,0,1/4
d42/m1/4,1/4,1/2
c42/m1/4,1/4,0
b42/m1/2,0,0
a42/m0,0,0

Harker planes:
Algebraic Normal vector A point in the plane
x-y,-x-y,1/2[0,0,1]0,0,1/2
2*x,2*y,0[0,0,1]0,0,0

Additional generators of Euclidean normalizer:
  Number of structure-seminvariant vectors and moduli: 2
    Vector    Modulus
    (1, 0, 0) 2
    (0, 0, 1) 2
  Further generators:
Matrix Rotation-part type Axis direction Screw/glide component Origin shift
x,-y,z -2[0,1,0]0,0,00,0,0

Grid factors implied by symmetries:
  Space group: (2, 2, 2)
  Structure-seminvariant vectors and moduli: (2, 1, 2)
  Euclidean normalizer: (2, 2, 2)

  All points of a grid over the unit cell are mapped
  exactly onto other grid points only if the factors
  shown above are factors of the grid.


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