Seiberg duality

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In quantum field theory, Seiberg duality, conjectured by Nathan Seiberg, is an S-duality relating two different supersymmetric QCDs. The two theories are not identical, but they agree at low energies. More precisely under a renormalization group flow they flow to the same IR fixed point, and so are in the same universality class.

It was first presented in Seiberg's 1994 article Electric-Magnetic Duality in Supersymmetric Non-Abelian Gauge Theories. It is an extension to nonabelian gauge theories with N=1 supersymmetry of Montonen–Olive duality in N=4 theories and electromagnetic duality in abelian theories.

The statement of Seiberg duality[edit]

Seiberg duality is an equivalence of the IR fixed points in an N=1 theory with SU(Nc) as the gauge group and Nf flavors of fundamental chiral multiplets and Nf flavors of antifundamental chiral multiplets in the chiral limit (no bare masses) and an N=1 chiral QCD with Nf-Nc colors and Nf flavors, where Nc and Nf are positive integers satisfying

N_f>N_c+1.

A stronger version of the duality relates not only the chiral limit but also the full deformation space of the theory. In the special case in which

{1\over 3}N_f < N_c < {2\over 3}N_f

the IR fixed point is a nontrivial interacting superconformal field theory. For a superconformal field theory, the anomalous scaling dimension of a chiral superfield D=\frac{3}{2} R where R is the R-charge. This is an exact result.

The dual theory contains a fundamental "meson" chiral superfield M which is color neutral but transforms as a bifundamental under the flavor symmetries.

SQCD dual theory
color gauge group SU(N_c) SU(N_f-N_c)
global internal symmetries SU(N_f)_L \times SU(N_f)_R \times U(1)_B \times U(1)_R SU(N_f)_L \times SU(N_f)_R \times U(1)_B \times U(1)_R
chiral superfields Q\,(N_f,1)_{1/N_c,(N_f-N_c)/N_f} \tilde{Q}\,(1,N_f)_{-1/(N_f-N_c),N_c/N_f}
Q^c\,(1,\overline{N_f})_{-1/N_c,(N_f-N_c)/N_f} \tilde{Q^c}\,(\overline{N_f},1)_{1/(N_f-N_c),N_c/N_f}
M\,(N_f,\overline{N_f})_{0,2(N_f-N_c)/N_f}

The dual theory contains the superpotential W=\alpha M \tilde{Q^c}\tilde{Q}.

Relations between the original and dual theories[edit]

Being an S-duality, Seiberg duality relates the strong coupling regime with the weak coupling regime, and interchanges chromoelectric fields (gluons) with chromomagnetic fields (gluons of the dual gauge group), and chromoelectric charges (quarks) with nonabelian 't Hooft–Polyakov monopoles. In particular, the Higgs phase is dual to the confinement phase as in the dual superconducting model.

The mesons and baryons are preserved by the duality. However in the electric theory the meson is a quark bilinear (M \equiv Q^c Q), while in the magnetic theory it is a fundamental field. In both theories the baryons are constructed from quarks, but the number of quarks in one baryon is the rank of the gauge group, which differs in the two dual theories.

The gauge symmetries of the theories do not agree, which is not problematic as the gauge symmetry is a feature of the formulation and not of the fundamental physics. The global symmetries relate distinct physical configurations and so they need to agree in any dual description.

Evidence for Seiberg duality[edit]

The moduli spaces of the dual theories are identical.

The global symmetries agree, as do the charges of the mesons and baryons.

In certain cases it reduces to ordinary electromagnetic duality.

It may be embedded in string theory via Hanany-Witten brane cartoons consisting of intersecting D-branes. There it is realized as the motion of an NS5-brane which is conjectured to preserve the universality class.

Six nontrivial anomalies may be computed on both sides of the duality, and they agree as they must in accordance with Gerard 't Hooft's anomaly matching conditions. The role of the additional fundamental meson superfield M in the dual theory is very crucial in matching the anomalies. The global gravitational anomalies also match up as the parity of the number of chiral fields is the same in both theories. The R-charge of the Weyl fermion in a chiral superfield is one less than the R-charge of the superfield. The R-charge of a gaugino is +1.

't Hooft anomaly matching conditions
anomaly SQCD dual theory
SU(N_f)_L^3 N_c d^{(3)}(N_f) N_c d^{(3)}(N_f)
SU(N_f)_L^2 U(1)_B d^{(2)}(N_f) d^{(2)}(N_f)
SU(N_f)_L^2 U(1)_R -\frac{N_c^2}{N_f}d^{(2)}(N_f) \frac{-N_c^2}{N_f}d^{(2)}(N_f)
U(1)_R -N_c^2 -1 -N_c^2 -1
U(1)_R^3 -2\frac{N_c^4}{N_f^2} + N_c^2 -1 -2\frac{N_c^4}{N_f^2} + N_c^2 -1
U(1)_B^2 U(1)_R -2 -2

Generalizations[edit]

Seiberg duality has been generalized in many directions. One generalization applies to quiver gauge theories, in which the flavor symmetries are also gauged. The simplest of these is a super QCD with the flavor group gauged and an additional term in the superpotential. It leads to a series of Seiberg dualities known as a duality cascade. It was introduced by Matthew Strassler and Igor Klebanov in Supergravity and a Confining Gauge Theory: Duality Cascades and \chiSB-Resolution of Naked Singularities.

It is not known whether Seiberg duality exists in 3-dimensional nonabelian gauge theories with only 4 supercharges, although a conjecture has appeared in Fractional M2-branes in some special cases with Chern–Simons terms.

References[edit]

Electric-Magnetic Duality in Supersymmetric Non-Abelian Gauge Theories by Nathan Seiberg.