Deconfining $\mathcal{N}=2$ SCFTs, or the Art of Brane Bending
We introduce a systematic approach to constructing $\mathcal{N}=1$ Lagrangians for a class of interacting $\mathcal{N}=2$ SCFTs. We analyse in detail the simplest case of the construction, arising from placing branes at an orientifolded $\mathbb{C}^2/\mathbb{Z}_2$ singularity. In this way we obtain...
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Zusammenfassung: | We introduce a systematic approach to constructing $\mathcal{N}=1$
Lagrangians for a class of interacting $\mathcal{N}=2$ SCFTs. We analyse in
detail the simplest case of the construction, arising from placing branes at an
orientifolded $\mathbb{C}^2/\mathbb{Z}_2$ singularity. In this way we obtain
Lagrangian descriptions for all the $R_{2,k}$ theories. The rank one theories
in this class are the $E_6$ Minahan-Nemeschansky theory and the $C_2\times
U(1)$ Argyres-Wittig theory. The Lagrangians that arise from our brane
construction manifestly exhibit either the entire expected flavour symmetry
group of the SCFT (for even $k$) or a full-rank subgroup thereof (for odd $k$),
so we can compute the full superconformal index of the $\mathcal{N}=2$ SCFTs,
and also systematically identify the Higgsings associated to partial closing of
punctures. |
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DOI: | 10.48550/arxiv.2111.08022 |