The continuously infinite group ∞1 is omitted.
| Coordinates | Seitz symbol |
|---|---|
| a, b, c | x, y, z | { 1 ‖ 1 | 0 } |
| -a, b, -c+1/2 | x, y, z | { 1 ‖ 2010 | 0 0 1/2 } |
| -a, -b, -c | -x, -y, -z | { -1 ‖ -1 | 0 } |
| a, -b, c+1/2 | -x, -y, -z | { -1 ‖ m010 | 0 0 1/2 } |
| a+1/2, b+1/2, c | x, y, z | { 1 ‖ 1 | 1/2 1/2 0 } |
| -a+1/2, b+1/2, -c+1/2 | x, y, z | { 1 ‖ 2010 | 1/2 1/2 1/2 } |
| -a+1/2, -b+1/2, -c | -x, -y, -z | { -1 ‖ -1 | 1/2 1/2 0 } |
| a+1/2, -b+1/2, c+1/2 | -x, -y, -z | { -1 ‖ m010 | 1/2 1/2 1/2 } |
| a, b, c | -x, y, z | { m ‖ 1 | 0 } |
| -a, b, -c+1/2 | -x, y, z | { m ‖ 2010 | 0 0 1/2 } |
| -a, -b, -c | x, -y, -z | { 2 ‖ -1 | 0 } |
| a, -b, c+1/2 | x, -y, -z | { 2 ‖ m010 | 0 0 1/2 } |
| a+1/2, b+1/2, c | -x, y, z | { m ‖ 1 | 1/2 1/2 0 } |
| -a+1/2, b+1/2, -c+1/2 | -x, y, z | { m ‖ 2010 | 1/2 1/2 1/2 } |
| -a+1/2, -b+1/2, -c | x, -y, -z | { 2 ‖ -1 | 1/2 1/2 0 } |
| a+1/2, -b+1/2, c+1/2 | x, -y, -z | { 2 ‖ m010 | 1/2 1/2 1/2 } |
| WP | Site symmetry | Representative |
|---|---|---|
| 4a | $\ce{^{-1}{-1}}\ce{^{\infty m}{1}} $ | (0,0,0 | 0,0,0) |
| 4b | $\ce{^{-1}{-1}}\ce{^{\infty m}{1}} $ | (0,1/2,0 | 0,0,0) |
| 4c | $\ce{^{-1}{-1}}\ce{^{\infty m}{1}} $ | (1/4,1/4,0 | 0,0,0) |
| 4d | $\ce{^{-1}{-1}}\ce{^{\infty m}{1}} $ | (1/4,1/4,1/2 | 0,0,0) |
| 4e | $\ce{^{1}{2}}\ce{^{\infty m}{1}} $ | (0,b,1/4 | 0,0,z) |
| 8f | $\ce{^{1}{1}}\ce{^{\infty m}{1}} $ | (a,b,c | 0,0,z) |
| Wavevector-k | Little co-group |
|---|---|
| A:(0,0,1/2) | $\ce{^{1}{2/}}\ce{^{-1}{m}}\ce{^{\infty m}{1}} $ |
| Γ:(0,0,0) | $\ce{^{1}{2/}}\ce{^{-1}{m}}\ce{^{\infty m}{1}} $ |
| M:(0,1,1/2) | $\ce{^{1}{2/}}\ce{^{-1}{m}}\ce{^{\infty m}{1}} $ |
| Y:(0,1,0) | $\ce{^{1}{2/}}\ce{^{-1}{m}}\ce{^{\infty m}{1}} $ |
| L:(1/2,1/2,1/2) | $\ce{^{-1}{-1}}\ce{^{\infty m}{1}} $ |
| V:(1/2,1/2,0) | $\ce{^{-1}{-1}}\ce{^{\infty m}{1}} $ |
| B:(u,0,w) | $\ce{^{m}{2/}}\ce{^{2}{m}}\ce{^{\infty}{1}} $ |
| Λ:(0,v,0) | $\ce{^{1}{2/}}\ce{^{-1}{m}}\ce{^{\infty}{1}} $ |
| U:(0,v,1/2) | $\ce{^{1}{2/}}\ce{^{-1}{m}}\ce{^{\infty}{1}} $ |
| GP:(u,v,w) | $\ce{^{-1}{-1}}\ce{^{\infty}{1}} $ |
Spin Brillouin Zone
| k-vector | k-vector-G↑ | A↑G(2) |
| Γ:(0,0,0) | Γ:(0,0,0) | $Γ_{1}^{S}(2) $ |
| A:(0,0,1/2) | A:(0,0,1/2) | $A_{1}^{S}(2) $ |
| L:(1/2,1/2,1/2) | L:(1/2,1/2,1/2) | $L_{1}^{S}(2) $ |
| M:(0,1,1/2) | M:(0,1,1/2) | $M_{1}^{S}(2) $ |
| V:(1/2,1/2,0) | V:(1/2,1/2,0) | $V_{1}^{S}(2) $ |
| Y:(0,1,0) | Y:(0,1,0) | $Y_{1}^{S}(2) $ |
| Λ:(0,v,0) | Λ:(0,v,0) | $Λ_{1}^{S}(2) $ |
| U:(0,v,1/2) | U:(0,v,1/2) | $U_{1}^{S}(2) $ |
| B:(u,0,w) | B:(u,0,w) | $B_{1}^{S}(2) $ |
| GP:(u,v,w) | GP:(u,v,w) | $GP_{1}^{S}(2) $ |
| k-vector | k-vector-G↑ | A↑G(4) |
| Γ:(0,0,0) | Γ:(0,0,0) | $Γ_{1}^{S}(2)⊕Γ_{2}^{S}(2) $ |
| A:(0,0,1/2) | A:(0,0,1/2) | $A_{1}^{S}(2)⊕A_{2}^{S}(2) $ |
| L:(1/2,1/2,1/2) | L:(1/2,1/2,1/2) | $2L_{1}^{S}(2) $ |
| M:(0,1,1/2) | M:(0,1,1/2) | $M_{1}^{S}(2)⊕M_{2}^{S}(2) $ |
| V:(1/2,1/2,0) | V:(1/2,1/2,0) | $2V_{1}^{S}(2) $ |
| Y:(0,1,0) | Y:(0,1,0) | $Y_{1}^{S}(2)⊕Y_{2}^{S}(2) $ |
| Λ:(0,v,0) | Λ:(0,v,0) | $Λ_{1}^{S}(2)⊕Λ_{2}^{S}(2) $ |
| U:(0,v,1/2) | U:(0,v,1/2) | $U_{1}^{S}(2)⊕U_{2}^{S}(2) $ |
| B:(u,0,w) | B:(u,0,w) | $2B_{1}^{S}(2) $ |
| GP:(u,v,w) | GP:(u,v,w) | $2GP_{1}^{S}(2) $ |