312
11 Spintronics
54600
54800
55000
55200
55400
55600
55800
56000
0
2
4
6
8
10
Frequency (GHz)
H (kgauss)
Spectrum for Exchange Interaction
1
Fig. 11.15 Modification of the F-section spectrum of Fig. 11.9 due to the D-term of the crystal
field spin-Hamiltonian of TiO 2 shown in (11.6)
A
1
2.5
6.3
1.6109
22.5489
32.1853
f
)
z
H
G
(
0.2
16.6685
Fig. 11.16 Relative absorption peaks versus frequency
11 Spintronics
54600
54800
55000
55200
55400
55600
55800
56000
0
2
4
6
8
10
Frequency (GHz)
H (kgauss)
Spectrum for Exchange Interaction
1
Fig. 11.15 Modification of the F-section spectrum of Fig. 11.9 due to the D-term of the crystal
field spin-Hamiltonian of TiO 2 shown in (11.6)
A
1
2.5
6.3
1.6109
22.5489
32.1853
f
)
z
H
G
(
0.2
16.6685
Fig. 11.16 Relative absorption peaks versus frequency