bcc-Fe and fcc-Ni and the Ni $6~{\mbox{eV}}$ satellite, in good agreement with XPS experimental results. [@re:Fe-expt-XPS1; @re:Ni-expt-XPS1]

The aim of the calculation for ferromagnetic bcc-Fe and fcc-Ni in this section is to see whether LDA+DMFT-IPT(1) scheme can reproduce a reasonable width of occupied 3d bands and Ni $6~{\mbox{eV}}$ satellite. In fact, we will show that LDA+DMFT-IPT(1) presents the width of occupied 3d bands for bcc-Fe and fcc-Ni and the $6~{\mbox{eV}}$ satellite in fcc-Ni to be in good agreement with both experimental ARPES [@re:Fe-expt-XPS1; @re:Ni-expt-XPS1] and also with previous LDA+DMFT results. [@re:Fe-Ni-UJ-paper; @re:Fe-Ni-KKR+DMFT]

Hamiltonian and $U$, $J$ values
-------------------------------

Lattice constants, atomic sphere radii in the TB-LMTO method and the averaged values of Coulomb and exchange interactions, $U$ and $J$, for ferromagnetic bcc-Fe and fcc-Ni to construct the Hamiltonian are summarized in Table \[tab:parameters\_and\_results\]. The values of $U$ and $J$ are obtained with the constraint-LDA calculation. [@re:Fe-Ni-UJ-paper] The basis set of the Hamiltonian consists of full valence bands of 4s, 4p and 3d orbitals, totally nine orbitals.

            lattice constant $a$ (Å)        atomic sphere radius $s_0$ (Å)             $U$ (eV)                     $J$ (eV)
  -------- ---------------------------- -------------------------------------- ------------------------- ------------------------------
   fcc-Ni             3.5233                            1.3768                  3.0[@re:Fe-Ni-UJ-paper]     0.9[@re:Fe-Ni-UJ-paper]
   bcc-Fe             2.8708                            1.4128                  2.0[@re:Fe-Ni-UJ-paper]     0.9[@re:Fe-Ni-UJ-paper]
    NiO               4.1948             1.2318 (Ni), 1.0699 (O), 