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X-MCD

X-MCD. X-MCD. Cu2+: 3d 9. X-MCD. m J =-5/2 to m J’ =-3/2. MCD. no LS. MCD. X-MCD. ++. +-. XAS. MCD. L3. 3 (*R 2 /9). 5. 8. +2. L2. 3. 1. 4. -2. m J =-5/2 to m J’ =-3/2. MCD. no LS. MCD. X-MCD. ++. +-. XAS. MCD. L3. 3 (*R 2 /9). 5. 8. +2. L2. 3. 1. 4.

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X-MCD

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  1. X-MCD

  2. X-MCD Cu2+: 3d9

  3. X-MCD mJ=-5/2 to mJ’=-3/2 MCD no LS MCD

  4. X-MCD ++ +- XAS MCD L3 3 (*R2/9) 5 8 +2 L2 3 1 4 -2 mJ=-5/2 to mJ’=-3/2 MCD no LS MCD

  5. X-MCD ++ +- XAS MCD L3 3 (*R2/9) 5 8 +2 L2 3 1 4 -2 mJ=-5/2 to mJ’=-3/2 MCD • No 3d spin-orbit coupling • No multiplets

  6. X-MCD MCD no LS MCD + crystal field

  7. X-MCD als7ni2a.rcg 10 14 2 4 1 1 INTER2 % shell03000000 spin03000000 orbit03000000 Add spin03 and orbit03 fields

  8. X-MCD Y % vertical 1 1 butler O3 to Oh to D4h to C4h endchain actor 0+ HAMILTONIAN ground PRINTEIG OPER HAMILTONIAN BRANCH 0+ > 0 0+ > 0+ > 0+ 1.0 OPER SHELL2 BRANCH 4+ > 0 0+ > 0+ > 0+ 0.0 BRANCH 4+ > 0 2+ > 0+ > 0+ 0.0 BRANCH 2+ > 0 2+ > 0+ > 0+ 0.0 OPER SPIN2 BRANCH 1+ > 0 1+ > ^0+ > 0+ 0.01 OPER ORBIT2 BRANCH 1+ > 0 1+ > ^0+ > 0+ 0.00 actor 0+ HAMILTONIAN excite PRINTEIG OPER HAMILTONIAN BRANCH 0+ > 0 0+ > 0+ > 0+ 1.0 OPER SHELL2 BRANCH 4+ > 0 0+ > 0+ > 0+ 0.0 BRANCH 4+ > 0 2+ > 0+ > 0+ 0.0 BRANCH 2+ > 0 2+ > 0+ > 0+ 0.0 OPER SPIN2 BRANCH 1+ > 0 1+ > ^0+ > 0+ 0.01 OPER ORBIT2 BRANCH 1+ > 0 1+ > ^0+ > 0+ 0.00 actor 1- left transi PRINTTRANS oper MULTIPOLE branch 1- > 0 1- > 1- > 1- 1.000 actor -1- right transi PRINTTRANS oper MULTIPOLE branch 1- > 0 1- > 1- > -1- 1.000 actor 0- parallel transi PRINTTRANS oper MULTIPOLE branch 1- > 0 1- > ^0- > 0- 1.000 RUN als7ni2a.rac

  9. Y % vertical 1 1 butler O3 to Oh to D4h to C4h endchain actor 0+ HAMILTONIAN ground PRINTEIG OPER HAMILTONIAN BRANCH 0+ > 0 0+ > 0+ > 0+ 1.0 OPER SHELL2 BRANCH 4+ > 0 0+ > 0+ > 0+ 0.0 BRANCH 4+ > 0 2+ > 0+ > 0+ 0.0 BRANCH 2+ > 0 2+ > 0+ > 0+ 0.0 OPER SPIN2 BRANCH 1+ > 0 1+ > ^0+ > 0+ 0.01 OPER ORBIT2 BRANCH 1+ > 0 1+ > ^0+ > 0+ 0.00 actor 0+ HAMILTONIAN excite PRINTEIG OPER HAMILTONIAN BRANCH 0+ > 0 0+ > 0+ > 0+ 1.0 OPER SHELL2 BRANCH 4+ > 0 0+ > 0+ > 0+ 0.0 BRANCH 4+ > 0 2+ > 0+ > 0+ 0.0 BRANCH 2+ > 0 2+ > 0+ > 0+ 0.0 OPER SPIN2 BRANCH 1+ > 0 1+ > ^0+ > 0+ 0.01 OPER ORBIT2 BRANCH 1+ > 0 1+ > ^0+ > 0+ 0.00 actor 1- left transi PRINTTRANS oper MULTIPOLE branch 1- > 0 1- > 1- > 1- 1.000 actor -1- right transi PRINTTRANS oper MULTIPOLE branch 1- > 0 1- > 1- > -1- 1.000 actor 0- parallel transi PRINTTRANS oper MULTIPOLE branch 1- > 0 1- > ^0- > 0- 1.000 RUN X-MCD als7ni2a.rac

  10. X-MCD als7ni2a.plo frame_title N2+ file b MCD -1- minus 1- addlines operator -1- spectrum operator 1- scale -1

  11. X-MCD MCD 3F4 LS 3F no LS

  12. X-MCD Z-pol (MJ=0) 3F4 LS left (MJ=-1) right (MJ=+1)

  13. X-MCD + crystal field + crystal field No LS

  14. X-MCD with charge transfer Ni parameters NiO parameters

  15. X-MCD in Ni2+

  16. X-MCD in Mn oxides

  17. Exercise: Charge Transfer on Mn3+ • Copy the rcg, rac, ban and plo files of als6ni2x1 to exct1 (or any other name) • Modify the calculation from Ni2+ to Mn3+. • Start by making the rcn-files for Mn 3d4 and Mn 3d5 ground states. Run TTRCN on them and replace the Ni parameters in the rcg-file with the Mn parameters. • Run TTRCG, TTRAC and TTBAN on the Mn files. • Plot the result • Modify exct1.ban in order to calculate • The pure 3d4 ground state • The pure 3d5 ground state • The spectrum of LaMnO3

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