Abstract

It is widely considered that the classical Higgs branch of 4d mathcal{N} = 2 SQCD is a well understood object. However there is no satisfactory understanding of its structure. There are two complications: (1) the Higgs branch chiral ring contains nilpotent elements, as can easily be checked in the case of SU(N) with 1 flavour. (2) the Higgs branch as a geometric space can in general be decomposed into two cones with nontrivial intersection, the baryonic and mesonic branches. To study the second point in detail we use the recently developed tool of magnetic quivers for five-brane webs, using the fact that the classical Higgs branch for theories with 8 supercharges does not change through dimensional reduction. We compare this approach with the computation of the hyper-Kähler quotient using Hilbert series techniques, finding perfect agreement if nilpotent operators are eliminated by the computation of a so called radical. We study the nature of the nilpotent operators and give conjectures for the Hilbert series of the full Higgs branch, giving new insights into the vacuum structure of 4d mathcal{N} = 2 SQCD. In addition we demonstrate the power of the magnetic quiver technique, as it allows us to identify the decomposition into cones, and provides us with the global symmetries of the theory, as a simple alternative to the techniques that were used to date.

Highlights

  • It is widely considered that the classical Higgs branch of 4d N = 2 SQCD is a well understood object

  • We study the nature of the nilpotent operators and give conjectures for the Hilbert series of the full Higgs branch, giving new insights into the vacuum structure of 4d N = 2 SQCD

  • In addition we demonstrate the power of the magnetic quiver technique, as it allows us to identify the decomposition into cones, and provides us with the global symmetries of the theory, as a simple alternative to the techniques that were used to date

Read more

Summary

Unitary gauge group

The Higgs branch Hilbert series can be found in all cases by combining the two following observations: 4Note that in the superpotential the same notation is used for the scalar components and for the corresponding chiral superfields. It is worth pointing out that the Higgs branch is in all cases the closure of a nilpotent orbit It can not be written as a union of several cones.. In order to compute the Higgs branch Hilbert series, one can use the technique known as hyper-Kahler quotient: one first computes the Hilbert series for the ring C[Q, Q]/ F-terms , weighted by fugacities of the gauge group, and performs a gauge integration to project on to the gauge invariant operators.

Special unitary gauge group
Decomposition in cones
Brane web method
General results
Brane webs and radical ideals
Finite factors and multiplicities
Mesonic branch
Nf even
Mesons and baryons
Baryonic branch
Future directions
A Tropical brane webs and magnetic quivers
C Some commutative algebra
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call