  We report the effects of heavy-ion irradiation on FeSe single crystals by
irradiating Uranium up to a dose equivalent matching field of $B_\phi$ = 16 T.
Almost continuous columnar defects along the $c$-axis with a diameter $\sim$10
nm are confirmed by high-resolution transmission electron microscopy. $T_c$ is
found to be suppressed by introducing columnar defects at a rate of
d$T_c$/d$B_\phi$ $\sim$ -0.29KT$^{-1}$, which is much larger than those
observed in iron pnictides. This unexpected large suppression of $T_c$ in FeSe
is discussed in relation to the large diameter of the columnar defects as well
as its unique band structure with a remarkably small Fermi energy. The critical
current density is first dramatically enhanced with irradiation reaching a
value over $\sim$2$\times$10$^5$ A/cm$^2$ ($\sim$5 times larger than that of
the pristine sample) at 2 K (self-field) with $B_\phi$ = 2 T, then gradually
suppressed with increasing $B_\phi$. The $\delta$$l$-pinning associated with
charge-carrier mean free path fluctuations, and the $\delta$$T_c$-pinning
associated with spatial fluctuations of the transition temperature are found to
coexist in the pristine FeSe, while the irradiation increases the contribution
from $\delta$$l$-pinning, and makes it dominant over $B_\phi$ = 4 T.
