Hermite-Einstein connections arise as solutions of the Hermitian Yang-Mills equations. These are a system of partial differential equations on a vector bundle over a Kähler manifold, which imply the Yang-Mills equations. Let be a Hermitian connection on a Hermitian vector bundle over a Kähler manifold of dimension. Then the Hermitian Yang-Mills equations are for some constant. Here we have Notice that since is assumed to be a Hermitian connection, the curvature is skew-Hermitian, and so implies. When the underlying Kähler manifold is compact, may be computed using Chern-Weil theory. Namely, we have Since and the identity endomorphism has trace given by the rank of, we obtain where is the slope of the vector bundle, given by and the volume of is taken with respect to the volume form. Due to the similarity of the second condition in the Hermitian Yang-Mills equations with the equations for an Einstein metric, solutions of the Hermitian Yang-Mills equations are often called Hermite-Einstein connections, as well as Hermitian Yang-Mills connections.
Examples
The Levi-Civita connection of a Kähler–Einstein metric is Hermite-Einstein with respect to the Kähler-Einstein metric. When the Hermitian vector bundle has a holomorphic structure, there is a natural choice of Hermitian connection, the Chern connection. For the Chern connection, the condition that is automatically satisfied. The Hitchin-Kobayashi correspondence asserts that a holomorphic vector bundle admits a Hermitian metric such that the associated Chern connection satisfies the Hermitian Yang-Mills equations if and only if the vector bundle is polystable. From this perspective, the Hermitian Yang-Mills equations can be seen as a system of equations for the metric rather than the associated Chern connection, and such metrics solving the equations are called Hermite-Einstein metrics. The Hermite-Einstein condition on Chern connections was first introduced by. These equation imply the Yang-Mills equations in any dimension, and in real dimension four are closely related to the self-dual Yang-Mills equations that define instantons. In particular, when the complex dimension of the Kähler manifold is, there is a splitting of the forms into self-dual and anti-self-dual forms. The complex structure interacts with this as follows: When the degree of the vector bundle vanishes, then the Hermitian Yang-Mills equations become. By the above representation, this is precisely the condition that. That is, is an ASD instanton. Notice that when the degree does not vanish, solutions of the Hermitian Yang-Mills equations cannot be anti-self-dual, and in fact there are no solutions to the ASD equations in this case.