The continuously infinite group ∞1 is omitted.
| Coordinates | Seitz symbol |
|---|---|
| a, b, c | x, y, z | { 1 ‖ 1 | 0 } |
| -b, a, c+1/4 | x, y, z | { 1 ‖ 4+001 | 0 0 1/4 } |
| b, -a, c+3/4 | x, y, z | { 1 ‖ 4-001 | 0 0 3/4 } |
| -a, -b, c+1/2 | x, y, z | { 1 ‖ 2001 | 0 0 1/2 } |
| a, b, c | -x, y, z | { m ‖ 1 | 0 } |
| -b, a, c+1/4 | -x, y, z | { m ‖ 4+001 | 0 0 1/4 } |
| b, -a, c+3/4 | -x, y, z | { m ‖ 4-001 | 0 0 3/4 } |
| -a, -b, c+1/2 | -x, y, z | { m ‖ 2001 | 0 0 1/2 } |
| WP | Site symmetry | Representative |
|---|---|---|
| 4a | $\ce{^{1}{1}}\ce{^{\infty m}{1}} $ | (a,b,c |0,0,z) |
| Wavevector-k | Little co-group |
|---|---|
| A:(1/2,1/2,1/2) | $\ce{^{1}{4}}\ce{^{\infty m}{1}} $ |
| Γ:(0,0,0) | $\ce{^{1}{4}}\ce{^{\infty m}{1}} $ |
| M:(1/2,1/2,0) | $\ce{^{1}{4}}\ce{^{\infty m}{1}} $ |
| Z:(0,0,1/2) | $\ce{^{1}{4}}\ce{^{\infty m}{1}} $ |
| R:(0,1/2,1/2) | $\ce{^{1}{2}}\ce{^{\infty m}{1}} $ |
| X:(0,1/2,0) | $\ce{^{1}{2}}\ce{^{\infty m}{1}} $ |
| Λ:(0,0,w) | $\ce{^{1}{4}}\ce{^{\infty}{1}} $ |
| V:(1/2,1/2,w) | $\ce{^{1}{4}}\ce{^{\infty}{1}} $ |
| D:(u,v,0) | $\ce{^{m}{2}}\ce{^{\infty}{1}} $ |
| Δ:(0,v,0) | $\ce{^{m}{2}}\ce{^{\infty}{1}} $ |
| E:(u,v,1/2) | $\ce{^{m}{2}}\ce{^{\infty}{1}} $ |
| S:(u,u,1/2) | $\ce{^{m}{2}}\ce{^{\infty}{1}} $ |
| Σ:(u,u,0) | $\ce{^{m}{2}}\ce{^{\infty}{1}} $ |
| T:(u,1/2,1/2) | $\ce{^{m}{2}}\ce{^{\infty}{1}} $ |
| U:(0,v,1/2) | $\ce{^{m}{2}}\ce{^{\infty}{1}} $ |
| W:(0,1/2,w) | $\ce{^{1}{2}}\ce{^{\infty}{1}} $ |
| Y:(u,1/2,0) | $\ce{^{m}{2}}\ce{^{\infty}{1}} $ |
| B:(0,v,w) | $\ce{^{1}{1}}\ce{^{\infty}{1}} $ |
| C:(u,u,w) | $\ce{^{1}{1}}\ce{^{\infty}{1}} $ |
| F:(u,1/2,w) | $\ce{^{1}{1}}\ce{^{\infty}{1}} $ |
| GP:(u,v,w) | $\ce{^{1}{1}}\ce{^{\infty}{1}} $ |
Spin Brillouin Zone
| k-vector | A↑G(4) |
| A:(1/2,1/2,1/2) | $A_{1}^{S}A_{3}^{S}(2)⊕A_{2}^{S}A_{4}^{S}(2) $ |
| Γ:(0,0,0) | $Γ_{1}^{S}(1)⊕Γ_{2}^{S}(1)⊕Γ_{3}^{S}Γ_{4}^{S}(2) $ |
| M:(1/2,1/2,0) | $M_{1}^{S}(1)⊕M_{2}^{S}(1)⊕M_{3}^{S}M_{4}^{S}(2) $ |
| Z:(0,0,1/2) | $Z_{1}^{S}Z_{3}^{S}(2)⊕Z_{2}^{S}Z_{4}^{S}(2) $ |
| R:(0,1/2,1/2) | $2R_{1}^{S}R_{2}^{S}(2) $ |
| X:(0,1/2,0) | $2X_{1}^{S}(1)⊕2X_{2}^{S}(1) $ |
| Λ:(0,0,w) | $Λ_{1}^{S}(1)⊕Λ_{2}^{S}(1)⊕Λ_{3}^{S}(1)⊕Λ_{4}^{S}(1) $ |
| V:(1/2,1/2,w) | $V_{1}^{S}(1)⊕V_{2}^{S}(1)⊕V_{3}^{S}(1)⊕V_{4}^{S}(1) $ |
| D:(u,v,0) | $4D_{1}^{S}(1) $ |
| Δ:(0,v,0) | $4Δ_{1}^{S}(1) $ |
| E:(u,v,1/2) | $2E_{1}^{S}E_{1}^{S}(2) $ |
| S:(u,u,1/2) | $2S_{1}^{S}S_{1}^{S}(2) $ |
| Σ:(u,u,0) | $4Σ_{1}^{S}(1) $ |
| T:(u,1/2,1/2) | $2T_{1}^{S}T_{1}^{S}(2) $ |
| U:(0,v,1/2) | $2U_{1}^{S}U_{1}^{S}(2) $ |
| W:(0,1/2,w) | $2W_{1}^{S}(1)⊕2W_{2}^{S}(1) $ |
| Y:(u,1/2,0) | $4Y_{1}^{S}(1) $ |
| B:(0,v,w) | $4B_{1}^{S}(1) $ |
| C:(u,u,w) | $4C_{1}^{S}(1) $ |
| F:(u,1/2,w) | $4F_{1}^{S}(1) $ |
| GP:(u,v,w) | $4GP_{1}^{S}(1) $ |