$U$. The spectrum shows electron affinity and ionization levels with different electron configurations of different occupation numbers and the system becomes insulating state at an integer filling in sufficiently large $U$. [@re:Fuji; @re:miura] IPT for multi orbitals was also proposed by Laad, Craco and Müller-Hartmann and applied to several realistic materials. [@re:MOIPT]

In this paper, we apply this DMFT with IPT scheme to realistic materials, where we adopt full LDA Hamiltonian without reducing its size and IPT as a solver for the mapped single impurity problem. In the following, we notify this DMFT with IPT as “LDA+DMFT-IPT(1)”. The goal of the present paper is as follows:

\(i) To generalize LDA+DMFT-IPT(1) which is applicable to various realistic strongly correlated materials, both metallic and insulating, multi-atom (compound), spin-polarized and strongly hybridized cases between s, p and d-bands.

\(ii) To apply LDA+DMFT-IPT(1) to ferromagnetic bcc-Fe and fcc-Ni and to antiferromagnetic NiO. For ferromagnetic bcc-Fe and fcc-Ni, we will discuss whether LDA+DMFT-IPT(1) reproduces the accurate width of occupied 3d bands and the observed satellite of spectrum at $6~{\mbox{eV}}$ below the Fermi energy in Ni (“$6~{\mbox{eV}}$ satellite”). Application of LDA+DMFT-IPT(1) to ferromagnetic bcc-Fe and fcc-Ni is a test in transition metals since previous LDA+DMFT [@re:Fe-Ni-UJ-paper; 