Carrier dynamics is crucial in semiconductors,
and it determines
their conductivity, response time, and overall functionality. In flat
bands (FBs), carriers with high effective masses are predicted to
host unconventional transport properties. The FBs usually overlap
with other trivial energy bands, however, making it difficult to accurately
distinguish their carrier dynamics. In this paper, we have investigated
the flat-band carrier dynamics of excited electrons in Nb3Cl8, which hosts ideal nonoverlapping FBs near the Fermi
level. The optical transition between Hubbard bands is abnormally
weakened, exhibiting weak interband absorption and its related slow
photoresponse with a time constant of ∼120 s, which are associated
with flat-band Mottness-induced large electron effective mass and
parity–forbidden transitions. Besides, the localized states
created by chlorine vacancies also act as trapping centers for carriers
with a time constant of ∼600 s, which are similar to those
of the compact localized states of the FB, making the relaxation behavior
even more extraordinary. The presence and impacts of atomic defects
are confirmed experimentally and theoretically. This work has revealed
the abnormal flat-band carrier dynamics of Nb3Cl8, which is essential for understanding the optical, electrical, and
thermal transport properties of flat-band materials.