  Low-energy excitations may manifest intricate behaviors of correlated
electron systems and provide essential insights into the dynamics of quantum
states and phase transitions. We study a two-orbital Hubbard model featuring
the so-called holon-doublon low-energy excitations in the Mott insulating
narrow band in the orbital-selective Mott phase (OSMP). We employ an improved
dynamical mean-field theory (DMFT) technique to calculate the spectral
functions at zero temperature. We show that the holon-doublon bound state is
not the sole component of the low-energy excitations. Instead, it should be a
bound state composed of a Kondo-like state in the wide band and a doublon in
the narrow band, named inter-band Kondo-like (IBK) bound states. Notably, as
the bandwidths of the two bands approach each other, we find anomalous IBK
bound-state excitations in the metallic {\em wide} band.
