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 ‖ m010 | 0 0 1/2 } |
| a, b+1/2, c+1/2 | -x, -y, -z | { -1 ‖ 1 | 0 1/2 1/2 } |
| a, -b+1/2, c | -x, -y, -z | { -1 ‖ m010 | 0 1/2 0 } |
| a, b, c | -x, y, z | { m ‖ 1 | 0 } |
| a, -b, c+1/2 | -x, y, z | { m ‖ m010 | 0 0 1/2 } |
| a, b+1/2, c+1/2 | x, -y, -z | { 2 ‖ 1 | 0 1/2 1/2 } |
| a, -b+1/2, c | x, -y, -z | { 2 ‖ m010 | 0 1/2 0 } |
| WP | Site symmetry | Representative |
|---|---|---|
| 2a | $\ce{^{-1}{m}}\ce{^{\infty m}{1}} $ | (a,1/4,c | 0,0,0) |
| 4b | $\ce{^{1}{1}}\ce{^{\infty m}{1}} $ | (a,b,c | 0,0,z) |
| Wavevector-k | Little co-group |
|---|---|
| A:(1/2,0,1/2) | $\ce{^{1}{m}}\ce{^{\infty /mm}{1}} $ |
| B:(0,0,1/2) | $\ce{^{1}{m}}\ce{^{\infty /mm}{1}} $ |
| C:(1/2,1/2,0) | $\ce{^{1}{m}}\ce{^{\infty /mm}{1}} $ |
| D:(0,1/2,1/2) | $\ce{^{1}{m}}\ce{^{\infty /mm}{1}} $ |
| E:(1/2,1/2,1/2) | $\ce{^{1}{m}}\ce{^{\infty /mm}{1}} $ |
| Γ:(0,0,0) | $\ce{^{1}{m}}\ce{^{\infty /mm}{1}} $ |
| Y:(1/2,0,0) | $\ce{^{1}{m}}\ce{^{\infty /mm}{1}} $ |
| Z:(0,1/2,0) | $\ce{^{1}{m}}\ce{^{\infty /mm}{1}} $ |
| F:(u,0,w) | $\ce{^{1}{m}}\ce{^{\infty 2}{1}} $ |
| G:(u,1/2,w) | $\ce{^{1}{m}}\ce{^{\infty 2}{1}} $ |
| Λ:(0,v,0) | $\ce{^{m}{m}}\ce{^{\infty 2}{1}} $ |
| U:(1/2,v,1/2) | $\ce{^{m}{m}}\ce{^{\infty 2}{1}} $ |
| V:(0,v,1/2) | $\ce{^{m}{m}}\ce{^{\infty 2}{1}} $ |
| W:(1/2,v,0) | $\ce{^{m}{m}}\ce{^{\infty 2}{1}} $ |
| GP:(u,v,w) | $\ce{^{1}{1}}\ce{^{\infty 2}{1}} $ |
Spin Brillouin Zone
| k-vector | A↑G(4) |
| A:(1/2,0,1/2) | $A_{1}^{S}A_{2}^{S}(4) $ |
| B:(0,0,1/2) | $B_{1}^{S}B_{2}^{S}(4) $ |
| C:(1/2,1/2,0) | $C_{1}^{S}(2)⊕C_{2}^{S}(2) $ |
| D:(0,1/2,1/2) | $D_{1}^{S}D_{2}^{S}(4) $ |
| E:(1/2,1/2,1/2) | $E_{1}^{S}E_{2}^{S}(4) $ |
| Γ:(0,0,0) | $Γ_{1}^{S}(2)⊕Γ_{2}^{S}(2) $ |
| Y:(1/2,0,0) | $Y_{1}^{S}(2)⊕Y_{2}^{S}(2) $ |
| Z:(0,1/2,0) | $Z_{1}^{S}(2)⊕Z_{2}^{S}(2) $ |
| F:(u,0,w) | $F_{1}^{S}(2)⊕F_{2}^{S}(2) $ |
| G:(u,1/2,w) | $G_{1}^{S}(2)⊕G_{2}^{S}(2) $ |
| Λ:(0,v,0) | $2Λ_{1}^{S}(2) $ |
| U:(1/2,v,1/2) | $U_{1}^{S}U_{1}^{S}(4) $ |
| V:(0,v,1/2) | $V_{1}^{S}V_{1}^{S}(4) $ |
| W:(1/2,v,0) | $2W_{1}^{S}(2) $ |
| GP:(u,v,w) | $2GP_{1}^{S}(2) $ |