Abstract

When spatial boundaries are inserted, SUSY can be broken. We show that in an N=2\mathcal{N}=2 supersymmetric theory, all the boundary conditions allowed by self-adjointness of the Hamiltonian break N=2\mathcal{N}=2 SUSY while only a few of these boundary conditions preserve N=1\mathcal{N}=1 SUSY. We also show that for a subset of the boundary conditions compatible with N=1\mathcal{N}=1 SUSY, there exist fermionic ground states which are localized near the boundary.

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