Table 1 Spin arrangements investigated for GdFeO3
From: Improper electric polarization in simple perovskite oxides with two magnetic sublattices
Gd spins | Fe spins | ||
|---|---|---|---|
G a | G b | G c | |
G a | Pn′a′21 Fe (Ga, Ab, Fc) Gd (Ga, Ab, Fc) Pc=−0.42 | P212121 Fe (Aa, Gb, Cc) Gd (Ga, Ab, Cc) P=0 | P21n′m′ Fe (Fa, Cb, Gc) Gd (Ga, Cb, 0) Pa<0.01 |
G b | P | Pna21 Fe (Aa, Gb, Cc) Gd (Aa, Gb, Cc) Pc=−0.41 | Pb |
G c | P | Pb21m Fe (Aa, Gb, Cc) Gd (0, 0, Gc) Pb<0.01 | Pn′a |
A a | P | Pna21 Fe (Aa, Gb, Cc) Gd (Aa, Gb, Cc) Pc<0.01 | Pb |
A b | Pn′a′21 Fe (Ga, Ab, Fc) Gd (Ga, Ab, Fc) Pc<0.01 | P212121 Fe (Aa, Gb, Cc) Gd (Ga, Ab, Cc) P=0 | P21n′m′ Fe (Fa, Cb, Gc) Gd (Fa, Ab, 0) Pa<0.01 |
A c | Pb′ | P21nm Fe (Aa, Gb, Cc) Gd (0, 0, Ac) Pa<0.01 | P21 |
C a | P | P21/c | P |
C b | P | P21/c | Pbn′m′ |
C c | P21/m | Pbnm | P21/c |
F a | P | P21/c | Pbn′m′ |
F b | P | P21/c | P |
F c | Pb′n′m | P21/m |
|

21 Fe (Ga, Ab, Fc) Gd (Aa, Gb, Fc) P=0
m′ Fe (Fa, Cb, Gc) Gd (Fa, Gb, 0) Pb<0.01
n′m Fe (Ga, Ab, Fc) Gd (0, 0, Gc) Pa<0.01
Fe (Fa, Cb, Gc) Gd (Fa, Cb, Gc) Pc=−0.41
21 Fe (Ga, Ab, Fc) Gd (Aa, Gb, Fc) P=0
m′ Fe (Fa, Cb, Gc) Gd (Aa, Cb, 0) Pb<0.01
m Fe (Ga, Ab, Fc) Gd (0, 0, Ac) 

Fe (Fa, Cb, Gc) Gd (Fa, Cb, Ac) P=0
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