  The magnetic response of the charged anyon fluid at temperatures lower and
larger than the fermion enery gap $\omega_{c}$ is investigated in the
self-consistent field approximation. We prove that the anyon system with
boundaries exhibits a total Meissner effect at temperatures smaller than the
fermion energy gap ($T\ll \omega_{c}$). The London penetration length at $T$
$\sim 200K$ is of the order $\lambda \sim 10^{-5}cm$. At $T\gg \omega_{c}$ a
new phase, characterized by an inhomogeneous magnetic penetration, is found. We
conclude that the energy gap, $\omega_{c},$ defines a scale that separates two
phases: a superconducting phase at $T\ll \omega_{c}$, and a non-superconducting
one at $T\gg \omega_{c}$.
