Abstract

The magnetic response of the charged anyon fluid at temperatures lower and larger than the fermion energy gap ωc 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≪ωc). The London penetration length at T∼200 K is of the order λ∼10−5 cm. At T≫ωc a new phase, characterized by an inhomogeneous magnetic penetration, is found. We conclude that the energy gap, ωc, defines a scale that separates two phases: a superconducting phase at T≪ωc, and a non-superconducting one at T≫ωc.

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