Abstract
We construct monopole operators for 3D Yang-Mills matter theories and Chern-Simons matter theories in canonical formalism. In this framework, monopole operators, although they are disorder operators, could be written in terms of the fundamental fields of the theory, and thus could be treated in the same way as the ordinary operators. We study the properties of the constructed monopole operators. In Chern-Simons matter theories, monopole operators transform as the local operators with the classical conformal dimension 0 under the action of the dilation and are also covariantly constant. In supersymmetric Chern-Simons matter theories like the ABJM model, monopole operators commute with all of the supercharges, and thus are SUSY invariant. The ABJM model with level $k=1,2$ is expected to have enhanced $SO(8)$ R symmetry due to the existence of the conserved extra R-symmetry currents ${j}_{\ensuremath{\mu}}^{AB}$ involving monopoles. With the explicit form of the monopole operators given, we prove the current conservation equation ${\ensuremath{\partial}}^{\ensuremath{\mu}}{j}_{\ensuremath{\mu}}^{AB}=0$ using the equations of motion. We also compute the extra $\mathcal{N}=2$ supercharges, derive the extra $\mathcal{N}=2$ SUSY transformation rules, and verify the closure of the $\mathcal{N}=8$ supersymmetry.
Highlights
AND SUMMARYIn any 3D gauge theory with the gauge group containing1 μνλ a Uð1Þ factor, there is a current Jμ 1⁄4 4π ε trFνλ whose conservation is equivalent to the Bianchi identity
In ABJM theory, monopole operators commute with the supercharges, while the anti-commutator of supercharges gives either a covariant derivative or a fielddependent gauge variation, so from Eq (9.27), one may conclude that monopole operators are both covariantly constant and invariant under that gauge variation
We show that the constructed monopole operators satisfy Eq (9.10), and so the global symmetry is enhanced to SOð8Þ
Summary
1 μνλ a Uð1Þ factor, there is a current Jμ 1⁄4 4π ε trFνλ whose conservation is equivalent to the Bianchi identity. In ABJM theory, the gauge-invariant combination of the monopole operators and the matter fields gives a new set of local operators carrying the vortex charge. In ABJM theory, monopole operators commute with the supercharges, while the anti-commutator of supercharges gives either a covariant derivative or a fielddependent gauge variation, so from Eq (9.27), one may conclude that monopole operators are both covariantly constant and invariant under that gauge variation The latter property could be stated as the algebraic identities for monopole operators and the matter fields. In this perspective, the symmetry enhancement comes from the classical symmetry of the Lagrangian together with the properties of the monopole operators.
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