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 ‖ 2100 | 0 0 1/2 } |
-a, b, -c | x, y, z | { 1 ‖ 2010 | 0 } |
-a, -b, c+1/2 | x, y, z | { 1 ‖ 2001 | 0 0 1/2 } |
-b, a, c+3/4 | -x, -y, -z | { -1 ‖ 4+001 | 0 0 3/4 } |
b, -a, c+1/4 | -x, -y, -z | { -1 ‖ 4-001 | 0 0 1/4 } |
b, a, -c+1/4 | -x, -y, -z | { -1 ‖ 2110 | 0 0 1/4 } |
-b, -a, -c+3/4 | -x, -y, -z | { -1 ‖ 21-10 | 0 0 3/4 } |
a, b, c | -x, y, z | { m ‖ 1 | 0 } |
a, -b, -c+1/2 | -x, y, z | { m ‖ 2100 | 0 0 1/2 } |
-a, b, -c | -x, y, z | { m ‖ 2010 | 0 } |
-a, -b, c+1/2 | -x, y, z | { m ‖ 2001 | 0 0 1/2 } |
-b, a, c+3/4 | x, -y, -z | { 2 ‖ 4+001 | 0 0 3/4 } |
b, -a, c+1/4 | x, -y, -z | { 2 ‖ 4-001 | 0 0 1/4 } |
b, a, -c+1/4 | x, -y, -z | { 2 ‖ 2110 | 0 0 1/4 } |
-b, -a, -c+3/4 | x, -y, -z | { 2 ‖ 21-10 | 0 0 3/4 } |
WP | Site symmetry | Representative |
---|---|---|
4a | $.\ce{^{1}{2}}.\ce{^{\infty m}{1}} $ | (0,b,0 | 0,0,z) |
4b | $.\ce{^{1}{2}}.\ce{^{\infty m}{1}} $ | (1/2,b,0 | 0,0,z) |
4c | $..\ce{^{-1}{2}}\ce{^{\infty m}{1}} $ | (a,a,5/8 | 0,0,0) |
8d | $\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{^{1}{2}}\ce{^{-1}{2}}\ce{^{\infty m}{1}} $ |
Γ:(0,0,0) | $\ce{^{-1}{4}}\ce{^{1}{2}}\ce{^{-1}{2}}\ce{^{\infty m}{1}} $ |
M:(1/2,1/2,0) | $\ce{^{-1}{4}}\ce{^{1}{2}}\ce{^{-1}{2}}\ce{^{\infty m}{1}} $ |
Z:(0,0,1/2) | $\ce{^{-1}{4}}\ce{^{1}{2}}\ce{^{-1}{2}}\ce{^{\infty m}{1}} $ |
R:(0,1/2,1/2) | $\ce{^{1}{2}}\ce{^{1}{2}}\ce{^{1}{2}}\ce{^{\infty m}{1}} $ |
X:(0,1/2,0) | $\ce{^{1}{2}}\ce{^{1}{2}}\ce{^{1}{2}}\ce{^{\infty m}{1}} $ |
Λ:(0,0,w) | $\ce{^{2}{4}}\ce{^{m}{2}}\ce{^{-1}{2}}\ce{^{\infty}{1}} $ |
V:(1/2,1/2,w) | $\ce{^{2}{4}}\ce{^{m}{2}}\ce{^{-1}{2}}\ce{^{\infty}{1}} $ |
Δ:(0,v,0) | $\ce{^{m}{2}}\ce{^{1}{2}}\ce{^{m}{2}}\ce{^{\infty}{1}} $ |
S:(u,u,1/2) | $\ce{^{-1}{2}}\ce{^{2}{2}}\ce{^{m}{2}}\ce{^{\infty}{1}} $ |
Σ:(u,u,0) | $\ce{^{-1}{2}}\ce{^{2}{2}}\ce{^{m}{2}}\ce{^{\infty}{1}} $ |
T:(u,1/2,1/2) | $\ce{^{1}{2}}\ce{^{m}{2}}\ce{^{m}{2}}\ce{^{\infty}{1}} $ |
U:(0,v,1/2) | $\ce{^{m}{2}}\ce{^{1}{2}}\ce{^{m}{2}}\ce{^{\infty}{1}} $ |
W:(0,1/2,w) | $\ce{^{m}{2}}\ce{^{m}{2}}\ce{^{1}{2}}\ce{^{\infty}{1}} $ |
Y:(u,1/2,0) | $\ce{^{1}{2}}\ce{^{m}{2}}\ce{^{m}{2}}\ce{^{\infty}{1}} $ |
B:(0,v,w) | $\ce{^{m}{2}}\ce{^{\infty}{1}} $ |
C:(u,u,w) | $\ce{^{-1}{2}}\ce{^{\infty}{1}} $ |
D:(u,v,0) | $\ce{^{m}{2}}\ce{^{\infty}{1}} $ |
E:(u,v,1/2) | $\ce{^{m}{2}}\ce{^{\infty}{1}} $ |
F:(u,1/2,w) | $\ce{^{m}{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_{3}^{S}(2) $ | |
A:(1/2,1/2,1/2) | R:(1/2,1/2,1/2) | $(A)R_{1}^{S}(4) $ | |
M:(1/2,1/2,0) | S:(1/2,1/2,0) | $(M)S_{1}^{S}(2)⊕(M)S_{3}^{S}(2) $ | |
R:(0,1/2,1/2) | T:(0,1/2,1/2) | $2 (R)T_{1}^{S}(2)$ | Spin Splitting |
X:(0,1/2,0) | Y:(0,1/2,0) | $2 (X)Y_{1}^{S}(1)⊕2 (X)Y_{3}^{S}(1)$ | Spin Splitting |
Z:(0,0,1/2) | Z:(0,0,1/2) | $Z_{1}^{S}(4) $ | |
Δ:(0,v,0) | Δ:(0,v,0) | $2Δ_{1}^{S}(1)⊕ 2Δ_{2}^{S}(1)$ | Spin Splitting |
Λ:(0,0,w) | Λ:(0,0,w) | $Λ_{1}^{S}(2)⊕Λ_{2}^{S}(2) $ | |
S:(u,u,1/2) | W:(u,u,1/2) | $(S)W_{1}^{S}W_{1}^{S}(4) $ | |
Σ:(u,u,0) | V:(u,u,0) | $2(Σ)V_{1}^{S}(2) $ | |
T:(u,1/2,1/2) | E:(u,1/2,1/2) | $2(T)E_{1}^{S}E_{2}^{S}(2)$ | Spin Splitting |
U:(0,v,1/2) | B:(0,v,1/2) | $2(U)B_{1}^{S}B_{2}^{S}(2)$ | Spin Splitting |
V:(1/2,1/2,w) | Q:(1/2,1/2,w) | $(V)Q_{1}^{S}(2)⊕(V)Q_{2}^{S}(2) $ | |
W:(0,1/2,w) | H:(0,1/2,w) | $2(W)H_{1}^{S}(1)⊕2(W)H_{2}^{S}(1)$ | Spin Splitting |
Y:(u,1/2,0) | C:(u,1/2,0) | $4(Y)C_{1}^{S}(1)$ | Spin Splitting |
B:(0,v,w) | K:(0,v,w) | $4(B)K_{1}^{S}(1)$ | Spin Splitting |
C:(u,u,w) | GP:(u,u,w) | $2(C)GP_{1}^{S}(2) $ | |
D:(u,v,0) | V:(u,v,0) | $4(D)V_{1}^{S}(1)$ | Spin Splitting |
E:(u,v,1/2) | W:(u,v,1/2) | $2(E)W_{1}^{S}W_{1}^{S}(2)$ | Spin Splitting |
F:(u,1/2,w) | N:(u,1/2,w) | $4(F)N_{1}^{S}(1)$ | Spin Splitting |
GP:(u,v,w) | GP:(u,v,w) | $4GP_{1}^{S}(1)$ | Spin Splitting |
k-vector | k-vector-G↑ | A↑G(4) | |
Γ:(0,0,0) | Γ:(0,0,0) | $Γ_{1}^{S}(2)⊕Γ_{3}^{S}(2) $ | |
A:(1/2,1/2,1/2) | R:(1/2,1/2,1/2) | $(A)R_{1}^{S}(4) $ | |
M:(1/2,1/2,0) | S:(1/2,1/2,0) | $(M)S_{2}^{S}(2)⊕(M)S_{4}^{S}(2) $ | |
R:(0,1/2,1/2) | T:(0,1/2,1/2) | $2 (R)T_{1}^{S}(2)$ | Spin Splitting |
X:(0,1/2,0) | Y:(0,1/2,0) | $2 (X)Y_{2}^{S}(1)⊕2 (X)Y_{4}^{S}(1)$ | Spin Splitting |
Z:(0,0,1/2) | Z:(0,0,1/2) | $Z_{1}^{S}(4) $ | |
Δ:(0,v,0) | Δ:(0,v,0) | $2Δ_{1}^{S}(1)⊕ 2Δ_{2}^{S}(1)$ | Spin Splitting |
Λ:(0,0,w) | Λ:(0,0,w) | $Λ_{1}^{S}(2)⊕Λ_{2}^{S}(2) $ | |
S:(u,u,1/2) | W:(u,u,1/2) | $(S)W_{1}^{S}W_{1}^{S}(4) $ | |
Σ:(u,u,0) | V:(u,u,0) | $2(Σ)V_{1}^{S}(2) $ | |
T:(u,1/2,1/2) | E:(u,1/2,1/2) | $2(T)E_{1}^{S}E_{2}^{S}(2)$ | Spin Splitting |
U:(0,v,1/2) | B:(0,v,1/2) | $2(U)B_{1}^{S}B_{2}^{S}(2)$ | Spin Splitting |
V:(1/2,1/2,w) | Q:(1/2,1/2,w) | $(V)Q_{1}^{S}(2)⊕(V)Q_{2}^{S}(2) $ | |
W:(0,1/2,w) | H:(0,1/2,w) | $2(W)H_{1}^{S}(1)⊕2(W)H_{2}^{S}(1)$ | Spin Splitting |
Y:(u,1/2,0) | C:(u,1/2,0) | $4(Y)C_{2}^{S}(1)$ | Spin Splitting |
B:(0,v,w) | K:(0,v,w) | $4(B)K_{1}^{S}(1)$ | Spin Splitting |
C:(u,u,w) | GP:(u,u,w) | $2(C)GP_{1}^{S}(2) $ | |
D:(u,v,0) | V:(u,v,0) | $4(D)V_{1}^{S}(1)$ | Spin Splitting |
E:(u,v,1/2) | W:(u,v,1/2) | $2(E)W_{1}^{S}W_{1}^{S}(2)$ | Spin Splitting |
F:(u,1/2,w) | N:(u,1/2,w) | $4(F)N_{1}^{S}(1)$ | Spin Splitting |
GP:(u,v,w) | GP:(u,v,w) | $4GP_{1}^{S}(1)$ | Spin Splitting |
k-vector | k-vector-G↑ | A↑G(8) | |
Γ:(0,0,0) | Γ:(0,0,0) | $Γ_{1}^{S}(2)⊕Γ_{2}^{S}(2)⊕Γ_{3}^{S}(2)⊕Γ_{4}^{S}(2) $ | |
A:(1/2,1/2,1/2) | R:(1/2,1/2,1/2) | $2(A)R_{1}^{S}(4) $ | |
M:(1/2,1/2,0) | S:(1/2,1/2,0) | $(M)S_{1}^{S}(2)⊕(M)S_{2}^{S}(2)⊕(M)S_{3}^{S}(2)⊕(M)S_{4}^{S}(2) $ | |
R:(0,1/2,1/2) | T:(0,1/2,1/2) | $4(R)T_{1}^{S}(2)$ | Spin Splitting |
X:(0,1/2,0) | Y:(0,1/2,0) | $2 (X)Y_{1}^{S}(1)⊕2 (X)Y_{2}^{S}(1)⊕2 (X)Y_{3}^{S}(1)⊕2 (X)Y_{4}^{S}(1)$ | Spin Splitting |
Z:(0,0,1/2) | Z:(0,0,1/2) | $2Z_{1}^{S}(4) $ | |
Δ:(0,v,0) | Δ:(0,v,0) | $4Δ_{1}^{S}(1)⊕4Δ_{2}^{S}(1)$ | Spin Splitting |
Λ:(0,0,w) | Λ:(0,0,w) | $2Λ_{1}^{S}(2)⊕2Λ_{2}^{S}(2) $ | |
S:(u,u,1/2) | W:(u,u,1/2) | $2(S)W_{1}^{S}W_{1}^{S}(4) $ | |
Σ:(u,u,0) | V:(u,u,0) | $4(Σ)V_{1}^{S}(2) $ | |
T:(u,1/2,1/2) | E:(u,1/2,1/2) | $4(T)E_{1}^{S}E_{2}^{S}(2)$ | Spin Splitting |
U:(0,v,1/2) | B:(0,v,1/2) | $4(U)B_{1}^{S}B_{2}^{S}(2)$ | Spin Splitting |
V:(1/2,1/2,w) | Q:(1/2,1/2,w) | $2(V)Q_{1}^{S}(2)⊕2(V)Q_{2}^{S}(2) $ | |
W:(0,1/2,w) | H:(0,1/2,w) | $4(W)H_{1}^{S}(1)⊕4(W)H_{2}^{S}(1)$ | Spin Splitting |
Y:(u,1/2,0) | C:(u,1/2,0) | $4(Y)C_{1}^{S}(1)⊕4(Y)C_{2}^{S}(1)$ | Spin Splitting |
B:(0,v,w) | K:(0,v,w) | $8(B)K_{1}^{S}(1)$ | Spin Splitting |
C:(u,u,w) | GP:(u,u,w) | $4(C)GP_{1}^{S}(2) $ | |
D:(u,v,0) | V:(u,v,0) | $8(D)V_{1}^{S}(1)$ | Spin Splitting |
E:(u,v,1/2) | W:(u,v,1/2) | $4(E)W_{1}^{S}W_{1}^{S}(2)$ | Spin Splitting |
F:(u,1/2,w) | N:(u,1/2,w) | $8(F)N_{1}^{S}(1)$ | Spin Splitting |
GP:(u,v,w) | GP:(u,v,w) | $8GP_{1}^{S}(1)$ | Spin Splitting |