The continuously infinite group ∞1 is omitted.
| Coordinates | Seitz symbol |
|---|---|
| a, b, c | x, y, z | { 1 ‖ 1 | 0 } |
| a, -b, c | -x, -y, -z | { -1 ‖ m010 | 0 } |
| a+1/2, b+1/2, c | x, y, z | { 1 ‖ 1 | 1/2 1/2 0 } |
| a+1/2, -b+1/2, c | -x, -y, -z | { -1 ‖ m010 | 1/2 1/2 0 } |
| a, b, c | -x, y, z | { m ‖ 1 | 0 } |
| a, -b, c | x, -y, -z | { 2 ‖ m010 | 0 } |
| a+1/2, b+1/2, c | -x, y, z | { m ‖ 1 | 1/2 1/2 0 } |
| a+1/2, -b+1/2, c | x, -y, -z | { 2 ‖ m010 | 1/2 1/2 0 } |
| WP | Site symmetry | Representative |
|---|---|---|
| 2a | $\ce{^{-1}{m}}\ce{^{\infty m}{1}} $ | (a,0,c | 0,0,0) |
| 4b | $\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}{m}}\ce{^{\infty m}{1}} $ |
| Γ:(0,0,0) | $\ce{^{-1}{m}}\ce{^{\infty m}{1}} $ |
| M:(0,1,1/2) | $\ce{^{-1}{m}}\ce{^{\infty m}{1}} $ |
| Y:(0,1,0) | $\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{^{2}{m}}\ce{^{\infty}{1}} $ |
| Λ:(0,v,0) | $\ce{^{-1}{m}}\ce{^{\infty}{1}} $ |
| U:(0,v,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) | Z:(0,0,1/2) | $(A)Z_{1}^{S}(2) $ | |
| L:(1/2,1/2,1/2) | U:(1/2,0,1/2) | $(L)U_{1}^{S}(2) $ | |
| M:(0,1,1/2) | R:(1/2,1/2,1/2) | $(M)R_{1}^{S}(2) $ | |
| V:(1/2,1/2,0) | X:(1/2,0,0) | $(V)X_{1}^{S}(2) $ | |
| Y:(0,1,0) | V:(1/2,1/2,0) | $(Y)V_{1}^{S}(2) $ | |
| Λ:(0,v,0) | GP:(v/2,v/2,0) | $(Λ)GP_{1}^{S}(2) $ | |
| U:(0,v,1/2) | GP:(v/2,v/2,1/2) | $(U)GP_{1}^{S}(2) $ | |
| B:(u,0,w) | GP:(u/2,-u/2,w) | $(B)GP_{1}^{S}(2) $ | |
| GP:(u,v,w) | GP:(u/2+v/2,-u/2+v/2,w) | $2 GP_{1}^{S}(1)$ | Spin Splitting |