Abstract

In (2+1) dimensions, the Maxwell term −(1/4)FαβFαβ-(1/4) F_{αβ}F^{αβ} can be replaced by the Chern-Simons three-form (κ/4)εαβγAαFβγ(κ/4)ε^{αβγ}A_αF_{βγ}, yielding a novel type of `electromagnetism'. This has been proposed for studying the Quantum Hall Effect as well as High-Temperature Superconductivity. The gauge field can be coupled to a scalar field either relativistically or non-relativistically. In both cases, one admits finite-energy, vortex solutions.

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