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Symmetry-adapted form of the Structure Factors


Magnetic Space Group: P-3m'1 (#164.89) [OG: P-3m'1 (#164.5.1319)]



Values of h, k, l:  h integer, k integer, l integer


Structure factors for general reflections (produced by centrings):


Diffraction vector type:   h,k,l
For any h,k,l:      I /= 0       F = (Fx,Fy,Fz)


Structure factors for special reflections:

Those diffraction vector types which are fully absent due to the general rule are not listed


Diffraction vector type:   0,0,l
For l = 1:      I = 0       F = (0,0,Fz)
For l = 2:      I = 0       F = (0,0,Fz)

Diffraction vector type:   2*h,-h,0
For h = 1:      I /= 0       F = (Fx,2*Fx,Fz)
For h = 2:      I /= 0       F = (Fx,2*Fx,Fz)

Diffraction vector type:   h,h,0
For h = 1:      I /= 0       F = (Fx,-Fx,Fz)
For h = 2:      I /= 0       F = (Fx,-Fx,Fz)

Diffraction vector type:   h,-2*h,0
For h = 1:      I /= 0       F = (2*Fy,Fy,Fz)
For h = 2:      I /= 0       F = (2*Fy,Fy,Fz)

Diffraction vector type:   0,k,l
For k = 1, l = 1:      I /= 0       F = (Fx,2*Fx,Fz)
For k = 1, l = 2:      I /= 0       F = (Fx,2*Fx,Fz)
For k = 2, l = 1:      I /= 0       F = (Fx,2*Fx,Fz)
For k = 2, l = 2:      I /= 0       F = (Fx,2*Fx,Fz)

Diffraction vector type:   h,-h,l
For h = 1, l = 1:      I /= 0       F = (Fx,-Fx,Fz)
For h = 1, l = 2:      I /= 0       F = (Fx,-Fx,Fz)
For h = 2, l = 1:      I /= 0       F = (Fx,-Fx,Fz)
For h = 2, l = 2:      I /= 0       F = (Fx,-Fx,Fz)

Diffraction vector type:   h,0,l
For h = 1, l = 1:      I /= 0       F = (2*Fy,Fy,Fz)
For h = 1, l = 2:      I /= 0       F = (2*Fy,Fy,Fz)
For h = 2, l = 1:      I /= 0       F = (2*Fy,Fy,Fz)
For h = 2, l = 2:      I /= 0       F = (2*Fy,Fy,Fz)


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