Table of Magnetic Space Group Symbols

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Extinction rules for the group R3m' (160.67)

Extinctions for general position (produced by centrings):

(h k l) -> Extinction rule/s: 2h + k + l ≠ 3n

    For  h = 1, k = 1, l = 1 :      I = 0       F = (0, 0, 0)

    For  h = 1, k = 1, l = 2 :      I = 0       F = (0, 0, 0)

    For  h = 1, k = 1, l = 3 :      I ≠ 0       F = (Fx, Fy, Fz)

    For  h = 1, k = 2, l = 1 :      I = 0       F = (0, 0, 0)

    For  h = 1, k = 2, l = 2 :      I ≠ 0       F = (Fx, Fy, Fz)

    For  h = 1, k = 2, l = 3 :      I = 0       F = (0, 0, 0)

    For  h = 1, k = 3, l = 1 :      I ≠ 0       F = (Fx, Fy, Fz)

    For  h = 1, k = 3, l = 2 :      I = 0       F = (0, 0, 0)

    For  h = 1, k = 3, l = 3 :      I = 0       F = (0, 0, 0)

    For  h = 2, k = 1, l = 1 :      I ≠ 0       F = (Fx, Fy, Fz)

    For  h = 2, k = 1, l = 2 :      I = 0       F = (0, 0, 0)

    For  h = 2, k = 1, l = 3 :      I = 0       F = (0, 0, 0)

    For  h = 2, k = 2, l = 1 :      I = 0       F = (0, 0, 0)

    For  h = 2, k = 2, l = 2 :      I = 0       F = (0, 0, 0)

    For  h = 2, k = 2, l = 3 :      I ≠ 0       F = (Fx, Fy, Fz)

    For  h = 2, k = 3, l = 1 :      I = 0       F = (0, 0, 0)

    For  h = 2, k = 3, l = 2 :      I ≠ 0       F = (Fx, Fy, Fz)

    For  h = 2, k = 3, l = 3 :      I = 0       F = (0, 0, 0)

    For  h = 3, k = 1, l = 1 :      I = 0       F = (0, 0, 0)

    For  h = 3, k = 1, l = 2 :      I ≠ 0       F = (Fx, Fy, Fz)

    For  h = 3, k = 1, l = 3 :      I = 0       F = (0, 0, 0)

    For  h = 3, k = 2, l = 1 :      I ≠ 0       F = (Fx, Fy, Fz)

    For  h = 3, k = 2, l = 2 :      I = 0       F = (0, 0, 0)

    For  h = 3, k = 2, l = 3 :      I = 0       F = (0, 0, 0)

    For  h = 3, k = 3, l = 1 :      I = 0       F = (0, 0, 0)

    For  h = 3, k = 3, l = 2 :      I = 0       F = (0, 0, 0)

    For  h = 3, k = 3, l = 3 :      I ≠ 0       F = (Fx, Fy, Fz)

Extinctions for special positions:

   (0 0 l)          ->      Extinction Rule/s: l any

   (0 k l)          ->      No extra extinctions found

   (h -h l)          ->      No extra extinctions found

   (h 0 l)          ->      No extra extinctions found

Go to the operators of 160.67 (R3m')
Go to the Wyckoff Positions of 160.67 (R3m')

Back to the list of magnetic space groups derived from R3m
Back to the list of Magnetic Space Groups

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