The resistivity around the ferromagnetic transition temperature in the doub
le-exchange model is studied by the Schwinger-boson approach. The spatial s
pin correlation responsible for scattering of conduction electrons are take
n into account by adopting the memory function formalism. Although the corr
elation shows a peak lower than the transition temperature, the resistivity
in the ferromagnetic state monotonically increases with increasing tempera
ture due to a variation of the electronic state of the conduction electron.
In the paramagnetic state, the resistivity is dominated by the short-range
correlation of scattering and is almost independent of the temperature. It
is attributed to a cancellation between the nearest-neighbor spin correlat
ion the fermion bandwidth, and the fermion kinetic energy. This result impl
ies the importance of the temperature dependence of the electronic states o
f the conduction electron as well as the localized spin states in both ferr
omagnetic and paramagnetic phases. [S0163-1829(99)08313-7].