Editing Supermultiplet (section)

=== N = 2 ===
The <math>\mathcal{N} = 2</math> '''vector''' or '''chiral multiplet''' <math>\Psi</math> contains a [[gauge field]] <math>A_\mu</math>, two [[Weyl fermion]]s <math>\lambda, \psi</math>, and a scalar <math>\phi</math> (which also transform in the [[adjoint representation]] of a [[gauge group]]). These can also be organised into a pair of <math>\mathcal{N} = 1</math> multiplets, an <math>\mathcal{N} = 1</math> vector multiplet <math>W = (A_\mu, \lambda)</math> and chiral multiplet <math>\Phi = (\phi, \psi)</math>. Such a multiplet can be used to define [[Seiberg–Witten theory]] concisely.

The <math>\mathcal{N} = 2</math> '''hypermultiplet''' or '''scalar multiplet''' consists of two Weyl fermions and two complex scalars, or two <math>\mathcal{N} = 1</math> chiral multiplets.