Abstract

We study the $\mathcal N=2$ field theory realized by D3-branes on the ${\mathbb C}^2/{\mathbb Z}_2$ orbifold. The dual supergravity solution exhibits a repulson singularity cured by the enhancon mechanism. By comparing the open and closed string descriptions of a probe D-instanton, we can compute the exact non-perturbative profile of the supergravity twisted field, which determines the supergravity background. We then show how the non-trivial IR physics of the field theory translates into the stringy effects that give rise to the enhancon mechanism and the associated excision procedure.

Highlights

  • Theory, which preserves N = 2 supersymmetry

  • We study the N = 2 field theory realized by D3-branes on the C2/Z2 orbifold

  • We show how the non-trivial IR physics of the field theory translates into the stringy effects that give rise to the enhancon mechanism and the associated excision procedure

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Summary

A supergravity perspective

Our setup is made up of a large number of parallel N regular and 2M fractional D3-branes in R4 × C × C2/Z2. Thinking of the fractional D3-branes as wrapped D5-branes, it is easy to understand that the reduction of the potentials C2 and B2 on the exceptional cycle Σ will give rise to non-zero twisted scalars c and b. These two fields can only depend on z, z, as the fractional D3-branes can only probe this plane, and are conveniently combined to form the complex field: γ. The profile of the twisted supergravity field is in turn solely determined by the positions of the fractional D3-branes. The distribution of branes is naturally related to the different vacua of the dual gauge theory, as we explain

A field theory perspective
Non-perturbative physics and the enhancon
The microscopic model
The four-dimensional gauge theory
The twisted supergravity field
The enhancon vacuum
A generic vacuum
Outlook
A Non-perturbative computation of the correlator
Full Text
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