The continuously infinite group ∞1 is omitted.
| Coordinates | Seitz symbol |
|---|---|
| a, b, c | x, y, z | { 1 ‖ 1 | 0 } |
| a+1/2, -b+1/2, c | x, y, z | { 1 ‖ m010 | 1/2 1/2 0 } |
| -a, -b, c | -x, -y, -z | { -1 ‖ 2001 | 0 } |
| -a+1/2, b+1/2, c | -x, -y, -z | { -1 ‖ m100 | 1/2 1/2 0 } |
| a, b, c | -x, y, z | { m ‖ 1 | 0 } |
| a+1/2, -b+1/2, c | -x, y, z | { m ‖ m010 | 1/2 1/2 0 } |
| -a, -b, c | x, -y, -z | { 2 ‖ 2001 | 0 } |
| -a+1/2, b+1/2, c | x, -y, -z | { 2 ‖ m100 | 1/2 1/2 0 } |
| WP | Site symmetry | Representative |
|---|---|---|
| 2a | $..\ce{^{-1}{2}}\ce{^{\infty m}{1}} $ | (0,0,c | 0,0,0) |
| 2b | $..\ce{^{-1}{2}}\ce{^{\infty m}{1}} $ | (0,1/2,c | 0,0,0) |
| 4c | $\ce{^{1}{1}}\ce{^{\infty m}{1}} $ | (a,b,c | 0,0,z) |
| Wavevector-k | Little co-group |
|---|---|
| Γ:(0,0,0) | $ \ce{^{-1}{m}}\ce{^{1}{m}}\ce{^{-1}{2}}\ce{^{\infty m}{1}} $ |
| R:(1/2,1/2,1/2) | $ \ce{^{-1}{m}}\ce{^{1}{m}}\ce{^{-1}{2}}\ce{^{\infty m}{1}} $ |
| S:(1/2,1/2,0) | $ \ce{^{-1}{m}}\ce{^{1}{m}}\ce{^{-1}{2}}\ce{^{\infty m}{1}} $ |
| T:(0,1/2,1/2) | $ \ce{^{-1}{m}}\ce{^{1}{m}}\ce{^{-1}{2}}\ce{^{\infty m}{1}} $ |
| U:(1/2,0,1/2) | $ \ce{^{-1}{m}}\ce{^{1}{m}}\ce{^{-1}{2}}\ce{^{\infty m}{1}} $ |
| X:(1/2,0,0) | $ \ce{^{-1}{m}}\ce{^{1}{m}}\ce{^{-1}{2}}\ce{^{\infty m}{1}} $ |
| Y:(0,1/2,0) | $ \ce{^{-1}{m}}\ce{^{1}{m}}\ce{^{-1}{2}}\ce{^{\infty m}{1}} $ |
| Z:(0,0,1/2) | $ \ce{^{-1}{m}}\ce{^{1}{m}}\ce{^{-1}{2}}\ce{^{\infty m}{1}} $ |
| A:(u,0,1/2) | $ \ce{^{-1}{m}}\ce{^{1}{m}}\ce{^{-1}{2}}\ce{^{\infty}{1}} $ |
| B:(0,v,1/2) | $ \ce{^{2}{m}}\ce{^{m}{m}}\ce{^{-1}{2}}\ce{^{\infty}{1}} $ |
| C:(u,1/2,0) | $ \ce{^{-1}{m}}\ce{^{1}{m}}\ce{^{-1}{2}}\ce{^{\infty}{1}} $ |
| D:(1/2,v,0) | $ \ce{^{2}{m}}\ce{^{m}{m}}\ce{^{-1}{2}}\ce{^{\infty}{1}} $ |
| Δ:(0,v,0) | $ \ce{^{2}{m}}\ce{^{m}{m}}\ce{^{-1}{2}}\ce{^{\infty}{1}} $ |
| E:(u,1/2,1/2) | $ \ce{^{-1}{m}}\ce{^{1}{m}}\ce{^{-1}{2}}\ce{^{\infty}{1}} $ |
| G:(1/2,0,w) | $ \ce{^{2}{m}}\ce{^{1}{m}}\ce{^{2}{2}}\ce{^{\infty}{1}} $ |
| H:(0,1/2,w) | $ \ce{^{2}{m}}\ce{^{1}{m}}\ce{^{2}{2}}\ce{^{\infty}{1}} $ |
| Λ:(0,0,w) | $ \ce{^{2}{m}}\ce{^{1}{m}}\ce{^{2}{2}}\ce{^{\infty}{1}} $ |
| P:(1/2,v,1/2) | $ \ce{^{2}{m}}\ce{^{m}{m}}\ce{^{-1}{2}}\ce{^{\infty}{1}} $ |
| Q:(1/2,1/2,w) | $ \ce{^{2}{m}}\ce{^{1}{m}}\ce{^{2}{2}}\ce{^{\infty}{1}} $ |
| Σ:(u,0,0) | $ \ce{^{-1}{m}}\ce{^{1}{m}}\ce{^{-1}{2}}\ce{^{\infty}{1}} $ |
| K:(0,v,w) | $ \ce{^{2}{m}}\ce{^{\infty}{1}} $ |
| L:(1/2,v,w) | $ \ce{^{2}{m}}\ce{^{\infty}{1}} $ |
| M:(u,0,w) | $ \ce{^{1}{m}}\ce{^{\infty}{1}} $ |
| N:(u,1/2,w) | $ \ce{^{1}{m}}\ce{^{\infty}{1}} $ |
| V:(u,v,0) | $ \ce{^{-1}{2}}\ce{^{\infty}{1}} $ |
| W:(u,v,1/2) | $ \ce{^{-1}{2}}\ce{^{\infty}{1}} $ |
| GP:(u,v,w) | $ \ce{^{1}{1}}\ce{^{\infty}{1}} $ |
Spin Brillouin Zone
| k-vector | k-vector-G↑ | A↑G(4) | |
| Γ:(0,0,0) | Γ:(0,0,0) | $Γ_{1}^{S}(2)⊕Γ_{2}^{S}(2) $ | |
| R:(1/2,1/2,-1/2) | E:(1/2,1/2,1/2) | $(R)E_{1}^{S}E_{2}^{S}(4) $ | |
| S:(1/2,1/2,0) | D:(0,1/2,1/2) | $(S)D_{1}^{S}D_{2}^{S}(4) $ | |
| T:(0,1/2,-1/2) | C:(1/2,1/2,0) | $(T)C_{1}^{S}(2)⊕(T)C_{2}^{S}(2) $ | |
| U:(1/2,0,-1/2) | A:(1/2,0,1/2) | $(U)A_{1}^{S}A_{2}^{S}(4) $ | |
| X:(1/2,0,0) | B:(0,0,1/2) | $(X)B_{1}^{S}B_{2}^{S}(4) $ | |
| Y:(0,1/2,0) | Z:(0,1/2,0) | $(Y)Z_{1}^{S}(2)⊕(Y)Z_{2}^{S}(2) $ | |
| Z:(0,0,-1/2) | Y:(1/2,0,0) | $(Z)Y_{1}^{S}(2)⊕(Z)Y_{2}^{S}(2) $ | |
| A:(u,0,1/2) | F:(-1/2,0,u) | $(A)F_{1}^{S}(2)⊕(A)F_{2}^{S}(2) $ | |
| B:(0,v,-1/2) | W:(1/2,v,0) | $2(B)W_{1}^{S}(2) $ | |
| C:(u,1/2,0) | G:(0,1/2,u) | $(C)G_{1}^{S}(2)⊕(C)G_{2}^{S}(2) $ | |
| D:(1/2,v,0) | V:(0,v,1/2) | $(D)V_{1}^{S}V_{1}^{S}(4) $ | |
| Δ:(0,v,0) | Λ:(0,v,0) | $2(Δ)Λ_{1}^{S}(2) $ | |
| E:(u,1/2,1/2) | G:(-1/2,1/2,u) | $(E)G_{1}^{S}(2)⊕(E)G_{2}^{S}(2) $ | |
| G:(1/2,0,w) | F:(-w,0,1/2) | $(G)F_{1}^{S}(2)⊕(G)F_{2}^{S}(2) $ | |
| H:(0,1/2,w) | G:(-w,1/2,0) | $(H)G_{1}^{S}(2)⊕(H)G_{2}^{S}(2) $ | |
| Λ:(0,0,w) | F:(-w,0,0) | $(Λ)F_{1}^{S}(2)⊕(Λ)F_{2}^{S}(2) $ | |
| P:(1/2,v,-1/2) | U:(1/2,v,1/2) | $(P)U_{1}^{S}U_{1}^{S}(4) $ | |
| Q:(1/2,1/2,w) | G:(-w,1/2,1/2) | $(Q)G_{1}^{S}(2)⊕(Q)G_{2}^{S}(2) $ | |
| Σ:(u,0,0) | F:(0,0,u) | $(Σ)F_{1}^{S}(2)⊕(Σ)F_{2}^{S}(2) $ | |
| K:(0,v,w) | GP:(-w,v,0) | $2(K)GP_{1}^{S}(2) $ | |
| L:(1/2,v,w) | GP:(-w,v,1/2) | $2(L)GP_{1}^{S}(2) $ | |
| M:(u,0,w) | F:(-w,0,u) | $2(M)F_{1}^{S}(1)⊕2(M)F_{2}^{S}(1)$ | Spin Splitting |
| N:(u,1/2,w) | G:(-w,1/2,u) | $2(N)G_{1}^{S}(1)⊕2(N)G_{2}^{S}(1)$ | Spin Splitting |
| V:(u,v,0) | GP:(0,v,u) | $2(V)GP_{1}^{S}(2) $ | |
| W:(u,v,1/2) | GP:(-1/2,v,u) | $2(W)GP_{1}^{S}(2) $ | |
| GP:(u,v,w) | GP:(-w,v,u) | $4GP_{1}^{S}(1)$ | Spin Splitting |