Review Article

Electronic Structure of Strongly Correlated Systems

Table 1

3 𝑑 orbital contribution to the formation of F e 𝐵 minority spin states with occupancy 𝑛 evaluated by diagonalization of the occupation matrix [155]. Although one of the 𝑡 2 𝑔 states of 𝐵 1 and 𝐵 4 sites is almost occupied with 𝑛 0 . 7 𝑒 the 𝑡 2 𝑔 minority spin occupancies of 𝐵 2 and 𝐵 3 F e 3 + cations are less than 0 . 1 𝑒 . The occupied 𝑡 2 𝑔 states of 𝐵 1 and 𝐵 4 F e 2 + cations are predominantly of 𝑑 𝑥 𝑧 ± 𝑑 𝑦 𝑧 and 𝑑 𝑥 2 𝑦 2 characters, respectively. The sum of 𝑡 2 𝑔  ( 𝑒 𝑔 ) occupations is given in the last column.

F e 𝐵 ionSym. 𝑡 2 𝑔 𝑒 𝑔 𝑡 2 𝑔
𝑦 𝑧 𝑧 𝑥 𝑥 2 𝑦 2 3 𝑧 2 𝑟 2 𝑥 𝑦 𝑛 ( 𝑒 𝑔 )

F e 𝐵 1 𝑎 𝑡 2 𝑔 −0.47−0.800.340.00−0.070.810.89
0.86−0.330.40−0.010.010.04
−0.210.490.84−0.010.040.04
𝑒 𝑔 0.040.060.01−0.49−0.870.150.26
−0.02−0.03−0.02−0.870.480.11

F e 𝐵 1 𝑏 𝑡 2 𝑔 −0.470.830.28−0.030.120.710.79
0.830.310.460.000.000.04
0.300.45−0.840.000.020.04
𝑒 𝑔 −0.05 0.110.020.55−0.830.150.27
0.01−0.040.000.830.550.12

F e 𝐵 2 𝑎 𝑡 2 𝑔 0.000.910.410.000.000.090.24
−0.990.000.010.000.000.08
−0.010.41−0.91−0.040.000.07
𝑒 𝑔 −0.010.000.000.000.990.270.52
0.00−0.020.04−0.990.000.25

F e 𝐵 2 𝑏 𝑡 2 𝑔 0.00 −0.90 0.450.010.000.090.23
−0.99 −0.01 −0.03 0.00−0.050.07
0.03 −0.45 −0.89 −0.040.000.07
𝑒 𝑔 0.00 −0.01 −0.040.990.000.260.52
−0.050.000.000.000.990.26

F e 𝐵 3 𝑡 2 𝑔 0.79−0.180.53−0.090.240.170.36
−0.220.730.630.13−0.100.11
0.520.65−0.55−0.08−0.040.08
𝑒 𝑔 −0.210.120.04−0.910.350.250.49
0.13−0.110.11−0.39−0.900.24

F e 𝐵 4 𝑡 2 𝑔 −0.55 −0.18 0.82 −0.02 0.020.800.87
0.51 −0.85 0.16 0.01 −0.04 0.04
0.660.500.55 −0.03 0.01 0.03
𝑒 𝑔 −0.01 −0.02 −0.03 −0.99 −0.12 0.130.25
−0.02 0.030.020.12 −0.99 0.11