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We present $mathcal{N}=2$ superconformal $mathsf{U}(1)$ duality-invariant models for an Abelian vector multiplet coupled to conformal supergravity. In a Minkowski background, such a nonlinear theory is expected to describe (the planar part of) the low-energy effective action for the $mathcal{N}=4$ $mathsf{SU}(N)$ super-Yang-Mills (SYM) theory on its Coulomb branch where (i) the gauge group $mathsf{SU}(N)$ is spontaneously broken to $mathsf{SU}(N-1) times mathsf{U}(1)$; and (ii) the dynamics is captured by a single $mathcal{N}=2$ vector multiplet associated with the $mathsf{U}(1)$ factor of the unbroken group. Additionally, a local $mathsf{U}(1)$ duality-invariant action generating the $mathcal{N}=2$ super-Weyl anomaly is proposed. By providing a new derivation of the recently constructed $mathsf{U}(1)$ duality-invariant $mathcal{N}=1$ superconformal electrodynamics, we introduce its $mathsf{SL}(2,{mathbb R})$ duality-invariant coupling to the dilaton-axion multiplet.
We construct a manifestly N=3 supersymmetric low-energy effective action of N=3 super Yang-Mills theory. The effective action is written in the N=3 harmonic superspace and respects the full N=3 superconformal symmetry. On mass shell this action is re
Superconformal indices (SCIs) of 4d ${mathcal N}=4$ SYM theories with simple gauge groups are described in terms of elliptic hypergeometric integrals. For $F_4, E_6, E_7, E_8$ gauge groups this yields first examples of integrals of such type. S-duali
In this note, I describe the space of vacua $mathcal{V}$ of four dimensional $mathcal{N}=4$ SYM on $mathbb{R}^4$ with gauge group a compact simple Lie Group $G$ as a stratified space. On each stratum, the low energy effective field theory is differen
We review the basic results concerning the structure of effective action in N=4 supersymmetric Yang-Mills theory in Coulomb phase. Various classical formulations of this theory are considered. We show that the low-energy effective action depending on
We continue the research initiated in hep-th/0607215 and apply our method of conformal automorphisms to generate various N=4 superconformal quantum many-body systems on the real line from a set of decoupled particles extended by fermionic degrees of