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. 2011 Mar 24;134(12):125105. doi: 10.1063/1.3564920

Table 1.

Definitions of the operators used in the diagonalization of the CE Hamiltonian [Eqs. 30, 42, 47].

Reference Definition Subspace
Equation 30 SΣz=12(S1z+S2z),SΣx=12(S1+S2++S1S2),SΣy=12i(S1+S2+S1S2), |1〉, |4〉, |5〉, |8〉
Equation 42 ESΣ=4SΣz2,SΣα=12ESΣ+SΣz,SΣβ=12ESΣSΣz,SΣ+=SΣx+iSΣy,SΣ=SΣxiSΣy  
Figure 5 SΔz=12(S1zS2z),SΔx=12(S1+S2+S1S2+),SΔy=12i(S1+S2S1S2+), |2〉, |3〉, |6〉, |7〉
  ESΔ=4SΔz2,SΔα=12ESΔ+SΔz,SΔβ=12ESΔSΔz,SΔ+=SΔx+iSΔy,SΔ=SΔxiSΔy  
     
Equation 47 MΣz=12(SΔz+ESΔIz),MΣx=12(SΔ+I++SΔI),MΣy=12i(SΔ+I+SΔI), |2˜,|7˜
Figure 6 EMΣ=4MΣz2,MΣα=12EMΣ+MΣz,MΣβ=12EMΣMΣz  
  MΔz=12(SΔzESΔIz),MΔx=12(SΔ+I+SΔI+),MΔy=12i(SΔ+ISΔI+),EMΔ=4MΔz2,MΔα=12EMΔ+MΔz,MΔβ=12EMΔMΔz |3˜,|6˜