The continuously infinite group ∞1 is omitted.
Coordinates | Seitz symbol |
---|---|
a, b, c | x, y, z | { 1 ‖ 1 | 0 } |
-b, a-b, c | x, y, z | { 1 ‖ 3+001 | 0 } |
-a+b, -a, c | x, y, z | { 1 ‖ 3-001 | 0 } |
-a, -a+b, c+1/2 | x, y, z | { 1 ‖ m210 | 0 0 1/2 } |
a-b, -b, c+1/2 | x, y, z | { 1 ‖ m120 | 0 0 1/2 } |
b, a, c+1/2 | x, y, z | { 1 ‖ m1-10 | 0 0 1/2 } |
a-b, a, c | -x, -y, -z | { -1 ‖ 6+001 | 0 } |
-a, -b, c | -x, -y, -z | { -1 ‖ 2001 | 0 } |
b, -a+b, c | -x, -y, -z | { -1 ‖ 6-001 | 0 } |
-a+b, b, c+1/2 | -x, -y, -z | { -1 ‖ m100 | 0 0 1/2 } |
-b, -a, c+1/2 | -x, -y, -z | { -1 ‖ m110 | 0 0 1/2 } |
a, a-b, c+1/2 | -x, -y, -z | { -1 ‖ m010 | 0 0 1/2 } |
a, b, c | -x, y, z | { m ‖ 1 | 0 } |
-b, a-b, c | -x, y, z | { m ‖ 3+001 | 0 } |
-a+b, -a, c | -x, y, z | { m ‖ 3-001 | 0 } |
-a, -a+b, c+1/2 | -x, y, z | { m ‖ m210 | 0 0 1/2 } |
a-b, -b, c+1/2 | -x, y, z | { m ‖ m120 | 0 0 1/2 } |
b, a, c+1/2 | -x, y, z | { m ‖ m1-10 | 0 0 1/2 } |
a-b, a, c | x, -y, -z | { 2 ‖ 6+001 | 0 } |
-a, -b, c | x, -y, -z | { 2 ‖ 2001 | 0 } |
b, -a+b, c | x, -y, -z | { 2 ‖ 6-001 | 0 } |
-a+b, b, c+1/2 | x, -y, -z | { 2 ‖ m100 | 0 0 1/2 } |
-b, -a, c+1/2 | x, -y, -z | { 2 ‖ m110 | 0 0 1/2 } |
a, a-b, c+1/2 | x, -y, -z | { 2 ‖ m010 | 0 0 1/2 } |
WP | Site symmetry | Representative |
---|---|---|
2a | $\ce{^{-1}{6}}..\ce{^{\infty m}{1}} $ | (0,0,c | 0,0,0) |
4b | $\ce{^{1}{3}}..\ce{^{\infty m}{1}} $ | (1/3,2/3,c | 0,0,z) |
6c | $\ce{^{-1}{2}}..\ce{^{\infty m}{1}} $ | (1/2,0,c | 0,0,0) |
12d | $\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}{6}}\ce{^{-1}{m}}\ce{^{1}{m}}\ce{^{\infty m}{1}} $ |
Γ:(0,0,0) | $\ce{^{-1}{6}}\ce{^{-1}{m}}\ce{^{1}{m}}\ce{^{\infty m}{1}} $ |
H:(1/3,1/3,1/2) | $\ce{^{-1}{6}}\ce{^{2}{m}}\ce{^{m}{m}}\ce{^{\infty}{1}} $ |
K:(1/3,1/3,0) | $\ce{^{-1}{6}}\ce{^{2}{m}}\ce{^{m}{m}}\ce{^{\infty}{1}} $ |
L:(1/2,0,1/2) | $\ce{^{1}{m}}\ce{^{2}{m}}\ce{^{2}{2}}\ce{^{\infty m}{1}} $ |
M:(1/2,0,0) | $\ce{^{1}{m}}\ce{^{2}{m}}\ce{^{2}{2}}\ce{^{\infty m}{1}} $ |
Δ:(0,0,w) | $\ce{^{2}{6}}\ce{^{2}{m}}\ce{^{1}{m}}\ce{^{\infty}{1}} $ |
P:(1/3,1/3,w) | $\ce{^{1}{3}}\ce{^{1}{1}}\ce{^{1}{m}}\ce{^{\infty}{1}} $ |
Λ:(u,u,0) | $\ce{^{1}{m}}\ce{^{-1}{m}}\ce{^{-1}{2}}\ce{^{\infty}{1}} $ |
Σ:(u,0,0) | $\ce{^{m}{m}}\ce{^{2}{m}}\ce{^{-1}{2}}\ce{^{\infty}{1}} $ |
Q:(u,u,1/2) | $\ce{^{1}{m}}\ce{^{-1}{m}}\ce{^{-1}{2}}\ce{^{\infty}{1}} $ |
R:(u,0,1/2) | $\ce{^{m}{m}}\ce{^{2}{m}}\ce{^{-1}{2}}\ce{^{\infty}{1}} $ |
U:(1/2,0,w) | $\ce{^{1}{m}}\ce{^{2}{m}}\ce{^{2}{2}}\ce{^{\infty}{1}} $ |
B:(u,v,0) | $\ce{^{-1}{2}}\ce{^{\infty}{1}} $ |
C:(u,u,w) | $\ce{^{1}{m}}\ce{^{\infty}{1}} $ |
D:(u,0,w) | $\ce{^{2}{m}}\ce{^{\infty}{1}} $ |
E:(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↑ | A1↑G(4) | |
A:(0,0,1/2) | A:(0,0,1/2) | $A_{1}^{S}A_{2}^{S}(4) $ | |
Γ:(0,0,0) | Γ:(0,0,0) | $Γ_{1}^{S}(2)⊕Γ_{2}^{S}(2) $ | |
H:(1/3,1/3,1/2) | H:(1/3,1/3,1/2) | $H_{3}^{S}(4) $ | |
K:(1/3,1/3,0) | K:(1/3,1/3,0) | $K_{3}^{S}(4) $ | |
L:(1/2,0,1/2) | L:(1/2,0,1/2) | $L_{1}^{S}L_{2}^{S}(4) $ | |
M:(1/2,0,0) | M:(1/2,0,0) | $M_{1}^{S}(2)⊕M_{2}^{S}(2) $ | |
B:(u,v,0) | B:(u,v,0) | $2B_{1}^{S}(2) $ | |
C:(u,u,w) | C:(u,u,w) | $2 C_{1}^{S}(1)⊕2 C_{2}^{S}(1)$ | Spin Splitting |
D:(u,0,w) | D:(u,0,w) | $2D_{1}^{S}(2) $ | |
Δ:(0,0,w) | Δ:(0,0,w) | $Δ_{1}^{S}(2)⊕Δ_{2}^{S}(2) $ | |
E:(u,v,1/2) | E:(u,v,1/2) | $2E_{1}^{S}(2) $ | |
GP:(u,v,w) | GP:(u,v,w) | $4GP_{1}^{S}(1)$ | Spin Splitting |
Λ:(u,u,0) | Λ:(u,u,0) | $Λ_{1}^{S}(2)⊕Λ_{2}^{S}(2) $ | |
P:(1/3,1/3,w) | P:(1/3,1/3,w) | $2P_{3}^{S}(2)$ | Spin Splitting |
Q:(u,u,1/2) | Q:(u,u,1/2) | $Q_{1}^{S}(2)⊕Q_{2}^{S}(2) $ | |
R:(u,0,1/2) | R:(u,0,1/2) | $R_{1}^{S}R_{1}^{S}(4) $ | |
Σ:(u,0,0) | Σ:(u,0,0) | $2Σ_{1}^{S}(2) $ | |
U:(1/2,0,w) | U:(1/2,0,w) | $U_{1}^{S}(2)⊕U_{2}^{S}(2) $ |
k-vector | k-vector-G↑ | A↑G(12) | |
A:(0,0,1/2) | A:(0,0,1/2) | $A_{1}^{S}A_{2}^{S}(4)⊕A_{3}^{S}A_{3}^{S}(8) $ | |
Γ:(0,0,0) | Γ:(0,0,0) | $Γ_{1}^{S}(2)⊕Γ_{2}^{S}(2)⊕2Γ_{3}^{S}(4) $ | |
H:(1/3,1/3,1/2) | H:(1/3,1/3,1/2) | $H_{1}^{S}(2)⊕H_{2}^{S}(2)⊕2H_{3}^{S}(4) $ | |
K:(1/3,1/3,0) | K:(1/3,1/3,0) | $K_{1}^{S}(2)⊕K_{2}^{S}(2)⊕2K_{3}^{S}(4) $ | |
L:(1/2,0,1/2) | L:(1/2,0,1/2) | $3 L_{1}^{S}L_{2}^{S}(4) $ | |
M:(1/2,0,0) | M:(1/2,0,0) | $3 M_{1}^{S}(2)⊕3 M_{2}^{S}(2) $ | |
B:(u,v,0) | B:(u,v,0) | $6B_{1}^{S}(2) $ | |
C:(u,u,w) | C:(u,u,w) | $6 C_{1}^{S}(1)⊕6 C_{2}^{S}(1)$ | Spin Splitting |
D:(u,0,w) | D:(u,0,w) | $6D_{1}^{S}(2) $ | |
Δ:(0,0,w) | Δ:(0,0,w) | $Δ_{1}^{S}(2)⊕Δ_{2}^{S}(2)⊕2Δ_{3}^{S}(4) $ | |
E:(u,v,1/2) | E:(u,v,1/2) | $6E_{1}^{S}(2) $ | |
GP:(u,v,w) | GP:(u,v,w) | $12GP_{1}^{S}(1)$ | Spin Splitting |
Λ:(u,u,0) | Λ:(u,u,0) | $3 Λ_{1}^{S}(2)⊕3 Λ_{2}^{S}(2) $ | |
P:(1/3,1/3,w) | P:(1/3,1/3,w) | $2 P_{1}^{S}(1)⊕2 P_{2}^{S}(1)⊕4P_{3}^{S}(2)$ | Spin Splitting |
Q:(u,u,1/2) | Q:(u,u,1/2) | $3 Q_{1}^{S}(2)⊕3 Q_{2}^{S}(2) $ | |
R:(u,0,1/2) | R:(u,0,1/2) | $3 R_{1}^{S}R_{1}^{S}(4) $ | |
Σ:(u,0,0) | Σ:(u,0,0) | $6Σ_{1}^{S}(2) $ | |
U:(1/2,0,w) | U:(1/2,0,w) | $3 U_{1}^{S}(2)⊕3 U_{2}^{S}(2) $ |