The lattice thermal conductivity (
\kappa _\rmlatt
) of mantle minerals plays a crucial role in the heat flow and temperature distribution within the Earth. MgSiO
3 akimotoite is stable at the bottom of the mantle transition zone; it transitions to MgSiO
3 perovskite (MgPv). In this work, we carry out a study of the
\kappa _\rmlatt
of MgSiO
3 akimotoite for pressures up to 25 GPa and temperatures up to 2500 K, based on first-principles calculations combined with lattice dynamics theory. At 300 K and 25 GPa, the
\kappa _\rmlatt
of MgSiO
3 akimotoite is 37.66 W m
–1 K
–1, larger than that of MgPv (13.46 W m
–1 K
–1), which implies that the phase transition explains the reduction in
\kappa _\rmlatt
. At 300 K, the pressure dependence of
\kappa _\rmlatt
is 0.68 W m
–1 K
–1 GPa
-1, stronger than that of MgPv (0.48 W m
–1 K
–1 GPa
-1). The azimuthal anisotropy in
\kappa _\rmlatt
of MgSiO
3 akimotoite decreases from 45.5% at 0 GPa to 28.94% at 25 GPa, while the variation trend is opposite to that of MgPv. In MgSiO
3 akimotoite, Fe incorporating in the mineral leads to a decrease in
\kappa _\rmlatt
and an increase in azimuthal anisotropy. Along the geotherm, the
\kappa _\rmlatt
of MgSiO
3 akimotoite is lower than that of ringwoodite, which would suggest that MgSiO
3 akimotoite slows down heat conduction at the bottom of mantle transition zone. These findings are useful for determining the thermal structure of, and understanding heat transfer in, the interior of the Earth.