Abstract

We consider D3 branes in presence of an S-fold plane. The latter is a non perturbative object, arising from the combined projection of an S-duality twist and a discrete orbifold of the R-symmetry group. This construction naively gives rise to 4d $\mathcal{N}=3$ SCFTs. Nevertheless it has been observed that in some cases supersymmetry is enhanced to $\mathcal{N}=4$. In this paper we study the explicit counting of degrees of freedom arising from vector multiplets associated to strings suspended between the D3 branes probing the S-fold. We propose that, for trivial discrete torsion, there is no vector multiplet associated to $(1,0)$ strings stretched between a brane and its image. We then focus on the case of rank 2 $\mathcal{N}=3$ theory that enhances to $SU(3)$ $\mathcal{N}=4$ SYM, explicitly spelling out the isomorphism between the BPS-spectrum of the manifestly $\mathcal{N}=3$ theory and that of three D3 branes in flat spacetime. Subsequently, we consider 3-pronged strings in these setups and show how wall-crossing in the S-fold background implies wall crossing in the flat geometry. This can be considered a consistency check of the \emph{conjectured} SUSY enhancement. We also find that the above isomorphism implies that a $(1,0)$ string, suspended between a brane and its image in the S-fold, corresponds to a 3-string junction in the flat geometry. This is in agreement with our claim on the absence of a vector multiplet associated to such $(1,0)$ strings. This is because the 3-string junction in flat geometry gives rise to a $1/4$-th BPS multiplet of the $\mathcal{N}=4$ algebra. Such multiplets always include particles with spin $>1$ as opposed to a vector multiplet which is restricted by the requirement that the spins must be $\leq 1$.

Highlights

  • In this paper we study the explicit counting of degrees of freedom arising from vector multiplets associated to strings suspended between the D3 branes probing the Sfold

  • We find that the above isomorphism implies that a (1, 0) string, suspended between a brane and its image in the S-fold, corresponds to a 3-string junction in the flat geometry

  • We develop a dictionary by mapping the masses and the charges associated to the (p, q) strings connecting the D3 branes in the S-fold geometry and the corresponding states in SU(3) N = 4 theory

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Summary

An explicit counting of the degrees of freedom

We start our analysis from the well known case of n D3 branes probing an O3 plane This corresponds to the Z2 projection in the language of the S-fold. 3.1 A lesson from the orientifold: the Z2 projection We consider a stack of n D3 branes on top of the O3− plane This gives rise to an N = 4, O(n) gauge theory. The spectrum of BPS-states in the theory is obtained by (p, q)strings stretched between the branes along the homotopically distinct paths that connect them. Each such state can be assigned a 4-vector of electromagnetic charges with respect to the U(1) gauge symmetry generated by the system of two branes. In the case of O3+-planes, such vector multiplets are there and we get an Sp(n) gauge group when all the branes are made coincident with the orientifold

Generalization to the Zk case
Warm-up
The case of the 3-pronged string
Wall crossing
Further directions and open questions
Full Text
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