Table 1 Energy contributions

From: Spin dynamics of the block orbital-selective Mott phase

 

\(\epsilon _{\mathrm{k}}\)

\(\epsilon _{\mathrm{U}}\)

\(\epsilon _{{\mathrm{U}}\prime }\)

\(\epsilon _{\mathrm{H}}\)

\(\epsilon _{\mathrm{P}}\)

Total

ω α

\(\left| {{\mathrm{GS}}} \right\rangle\)

−0.027

8.006

15.280

−1.055

−0.010

22.194

 

\(\left| {\mathrm{A}} \right\rangle\)

0.007

7.993

15.280

−1.065

−0.009

22.206

0.012

\(\left| {\mathrm{O}} \right\rangle\)

−0.031

8.081

15.262

−0.946

−0.016

22.350

0.156

  1. Kinetic, intra- and inter-orbital interaction, Hund, and pair-hopping energy contributions to the energy of given eigenstates. The last column shows the difference between \(\left| {{\mathrm{GS}}} \right\rangle\) and states within the acoustic (red color) and optical (green color) modes. Results are obtained for L = 4 and U/W = 0.8, using the Lanczos method. All numbers in units of eV