2019年1月25日
3d "chiral" Kutasov-Schwimmer duality
- 記述言語
- 掲載種別
- 機関テクニカルレポート,技術報告書,プレプリント等
We propose a "chiral" version of the Kutasov-Schwimmer duality in a 3d<br />
$\mathcal{N}=2$ $SU(N)$ gauge theory with $F$ fundamental matters, $\bar{F}$<br />
anti-fundamental matters and an adjoint matter $X$ with a tree-level<br />
superpotential $W= \mathrm{tr} \, X^{k+1}$. The theory exhibits a rich<br />
structure of the baryonic and (dressed) Coulomb branch operators. At first<br />
sight, the duality seems bad due to the mismatch of the anti-baryonic branch in<br />
the moduli space of vacua. The duality well works by realizing that the<br />
anti-baryonic operators are identified with some of the dressed Coulomb branch<br />
coordinates under the proposed duality. This generalizes the $SU(N)$ ``chiral''<br />
duality with (anti-)fundamental matters, which we previously proposed.
$\mathcal{N}=2$ $SU(N)$ gauge theory with $F$ fundamental matters, $\bar{F}$<br />
anti-fundamental matters and an adjoint matter $X$ with a tree-level<br />
superpotential $W= \mathrm{tr} \, X^{k+1}$. The theory exhibits a rich<br />
structure of the baryonic and (dressed) Coulomb branch operators. At first<br />
sight, the duality seems bad due to the mismatch of the anti-baryonic branch in<br />
the moduli space of vacua. The duality well works by realizing that the<br />
anti-baryonic operators are identified with some of the dressed Coulomb branch<br />
coordinates under the proposed duality. This generalizes the $SU(N)$ ``chiral''<br />
duality with (anti-)fundamental matters, which we previously proposed.
- ID情報
-
- arXiv ID : arXiv:1901.08642