nLab
quiver gauge theory

Contents

Context

Quantum field theory

String theory

Contents

Idea

General

A quiver gauge theory is a gauge theory – usually a super Yang-Mills theory – whose field content is determined by a quiver in that to each node x ix_i of the quiver is assigned a gauge group U(n i)U(n_i) and to each edge a fermion field species which is charged as the fundamental representation under the gauge group of the target and the anti-fundamental representation of the domain of the quiver edge.

Such data naturally arises in geometric engineering of quantum field theory from D-brane models in string theory with D-branes located at certain singularities of a Calabi-Yau variety: the nodes x ix_i of the quiver for a (d+1)(d+1)-dimensional quiver gauge theory correspond to n in_i coincident dd-D-branes and the edges of the quiver to open string states stretching between these branes. Under this interpretation, a representation of the quiver corresponds to giving all these fields a vacuum expectation value.

As fixed point locus

Consider a U(N)U(N) Chan-Paton gauge field theory on D-branes at a GG-orbifold singularity nG\mathbb{C}^n\sslash G for Γ\Gamma a finite group.

Then the fermions transform in c(N[r])(Nr *)\mathbf{c} \otimes (N \mathbf[r]) \otimes (N \mathbf{r}^\ast), where r\mathbf{r} denotes the regular representation of Γ\Gamma and c\mathbf{c} denotes the representation which defines the orbifold action.

Then the Γ\Gamma-fixed point space inside this representation is

(c(Nr)(Nr *)) Γ \big( \mathbf{c} \otimes (N \mathbf{r}) \otimes (N \mathbf{r}^\ast) \big)^\Gamma

is the corresponding weighted McKay quiver matrix.

This observation is due to Lawrence-Nekrasov-Vafa 98, Section 2.1

Properties

Relation between coherent sheaves and quiver representations

The representation theoretic aspects of the gauge theory thus obtained depend only on aspects which are already seen by the B-model topological string, which in this context plays the role of a simplified version of the physical superstring itself. By the discussion at TCFT this topological field theory is essentially determined by its derived category of B-branes, which is a derived category of coherent sheaves on the given target spacetime. Localized to suitable singularities the B-branes decompose into fractional branes which is mathematically reflected by the existence of exceptional collections of objects in the derived category. The endomorphism algebra of the direct sum of the objects in the exceptional collection turns out to be the path algebra of the corresponding quiver and under this identification the derived categories of coherent sheaves and of quiver representations are equivalent (Bondal 90). This equivalence to quiver representations gives one of the ways of getting a concrete combinatorial handle on derived categories of B-branes and hence on properties of quiver gauge theory.

Relation to Seiberg duality

Under geometric engineering of quantum field theory via D-branes situated at ADE-singularities in non-compact Calabi-Yau varieties as above, for instance Seiberg duality of the corresponding quiver gauge field theories may be understood in terms of equivalences of categories of derived quiver representations corresponding to mutations of exceptional collections? etc. (Robles-Llana & Rocek 04).

References

General

An original article is

The understanding of the McKay quiver as the fixed point space in the fermion-representation under R-symmetry is due to

In

  • Alexei Bondal, Helices, representations of quivers and Koszul algebras, in Helices and vector bundles, vol. 148 of London Math. Soc. Lecture Note Ser., pp. 75–95. Cambridge Univ. Press, Cambridge, 1990.

an exceptional collection in the derived category of coherent sheaves on a suitable Calabi-Yau variety cone is used to induce a quiver and make the derived category be equivalent to that of its quiver representations.

Review and discussion of further details includes

With emphasis on string phenomenology:

Discussion from the point of view of worldsheet 2d CFT is in

Discussion for Sasakian manifolds includes

Seiberg duality

Last revised on February 14, 2019 at 09:28:41. See the history of this page for a list of all contributions to it.