Table 1 Calculated anomalous Hall conductivity for different noncollinear antiferromagnetic phases.

Spin	Energy/f.u.	σ_x	σ_y
configuration	(meV)	(S ⋅ cm⁻¹)	(S ⋅ cm⁻¹)
\({a}_{1}^{+}\)	0	0	0
\({a}_{1}^{-}\,\,(\phi =9{0}^{o})\)	−4.472	−226	0
\({a}_{2}^{-}\,\,(\phi =21{0}^{o})\)	−4.472	116	−204
\({a}_{3}^{-}\,\,(\phi =33{0}^{o})\)	−4.472	116	204
\({a}_{4}^{-}\, \, (\phi ={0}^{o})\)	−4.451	0	223
\({a}_{5}^{-}\,\,(\phi =3{0}^{o})\)	−4.472	−116	204
\({a}_{6}^{-}\,\,(\phi =6{0}^{o})\)	−4.451	−200	−104
\({a}_{7}^{-}\,\,(\phi =9{0}^{o})\)	−4.472	−226	0

The stability energies of vector chirality κ = − 1 noncollinear antiferromagnetic states with respect to κ = + 1 one and the corresponding intrinsic anomalous Hall conductivity, σ_x(y). The angle ϕ in parenthesis is defined with respect to the \({a}_{4}^{-}\) antiferromagnetic configuration, representing uniform spin rotation measured in integer multiple of 30°.

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