Information of spin space group $C\ce{^{1}{c}}\ce{^{\text{-}1}{(0 \ 0 \ 1/2)}}\ce{^{\infty m}{1}}$ ( nSSG:9.8.2.1 )

General Positions

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 ‖ m010 | 0 0 1/2 }
a+1/2, b+1/2, c | x, y, z	{ 1 ‖ 1 | 1/2 1/2 0 }
a+1/2, -b+1/2, c+1/2 | x, y, z	{ 1 ‖ m010 | 1/2 1/2 1/2 }
a, b, c+1/2 | -x, -y, -z	{ -1 ‖ 1 | 0 0 1/2 }
a, -b, c | -x, -y, -z	{ -1 ‖ m010 | 0 }
a+1/2, b+1/2, c+1/2 | -x, -y, -z	{ -1 ‖ 1 | 1/2 1/2 1/2 }
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+1/2 | -x, y, z	{ m ‖ m010 | 0 0 1/2 }
a+1/2, b+1/2, c | -x, y, z	{ m ‖ 1 | 1/2 1/2 0 }
a+1/2, -b+1/2, c+1/2 | -x, y, z	{ m ‖ m010 | 1/2 1/2 1/2 }
a, b, c+1/2 | x, -y, -z	{ 2 ‖ 1 | 0 0 1/2 }
a, -b, c | x, -y, -z	{ 2 ‖ m010 | 0 }
a+1/2, b+1/2, c+1/2 | x, -y, -z	{ 2 ‖ 1 | 1/2 1/2 1/2 }
a+1/2, -b+1/2, c | x, -y, -z	{ 2 ‖ m010 | 1/2 1/2 0 }

Wyckoff Positions

WP	Site symmetry	Representative
4a	$\ce{^{-1}{m}}\ce{^{\infty m}{1}} $	(a,0,c | 0,0,0)
8b	$\ce{^{1}{1}}\ce{^{\infty m}{1}} $	(a,b,c | 0,0,z)

Spin Brillouin Zone & k-little co-groups

Wavevector-k	Little co-group
A:(0,0,1/2)	$\ce{^{1}{m}}\ce{^{\infty /mm}{1}} $
Γ:(0,0,0)	$\ce{^{1}{m}}\ce{^{\infty /mm}{1}} $
M:(0,1,1/2)	$\ce{^{1}{m}}\ce{^{\infty /mm}{1}} $
Y:(0,1,0)	$\ce{^{1}{m}}\ce{^{\infty /mm}{1}} $
L:(1/2,1/2,1/2)	$\ce{^{1}{1}}\ce{^{\infty /mm}{1}} $
V:(1/2,1/2,0)	$\ce{^{1}{1}}\ce{^{\infty /mm}{1}} $
B:(u,0,w)	$\ce{^{1}{m}}\ce{^{\infty 2}{1}} $
Λ:(0,v,0)	$\ce{^{m}{m}}\ce{^{\infty 2}{1}} $
U:(0,v,1/2)	$\ce{^{m}{m}}\ce{^{\infty 2}{1}} $
GP:(u,v,w)	$\ce{^{1}{1}}\ce{^{\infty 2}{1}} $

Spin Brillouin Zone

Band Representations (Magnon)

8b

k-vector	A↑G(4)
A:(0,0,1/2)	$A_{1}^{S}A_{2}^{S}(4) $
Γ:(0,0,0)	$Γ_{1}^{S}(2)⊕Γ_{2}^{S}(2) $
M:(0,1,1/2)	$M_{1}^{S}M_{2}^{S}(4) $
Y:(0,1,0)	$Y_{1}^{S}(2)⊕Y_{2}^{S}(2) $
L:(1/2,1/2,1/2)	$2L_{1}^{S}(2) $
V:(1/2,1/2,0)	$2V_{1}^{S}(2) $
B:(u,0,w)	$B_{1}^{S}(2)⊕B_{2}^{S}(2) $
GP:(u,v,w)	$2GP_{1}^{S}(2) $
Λ:(0,v,0)	$2Λ_{1}^{S}(2) $
U:(0,v,1/2)	$U_{1}^{S}U_{1}^{S}(4) $