In mathematics, and in particular gauge theory and complex geometry, a Hermitian Yang–Mills connection (or Hermite–Einstein connection) is a Chern connection associated to an inner product on a holomorphic vector bundle over a Kähler manifold that satisfies an analogue of Einstein's equations: namely, the contraction of the curvature 2-form of the connection with the Kähler form is required to be a constant times the identity transformation. Hermitian Yang–Mills connections are special examples of Yang–Mills connections, and are often called instantons. The Kobayashi–Hitchin correspondence proved by Donaldson, Uhlenbeck and Yau asserts that a holomorphic vector bundle over a compact Kähler manifold admits a Hermitian Yang–Mills connection if and only if it is slope polystable.
Hermitian Yang–Mills equations 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 A {\displaystyle A} be a Hermitian connection on a Hermitian vector bundle E {\displaystyle E} over a Kähler manifold X {\displaystyle X} of dimension n {\displaystyle n} . Then the Hermitian Yang–Mills equations are:
F A 0 , 2 = 0 F A ⋅ ω = λ ( E ) Id , {\displaystyle {\begin{aligned}&F_{A}^{0,2}=0\\&F_{A}\cdot \omega =\lambda (E)\operatorname {Id} ,\end{aligned}}}
for some constant λ ( E ) ∈ C {\displaystyle \lambda (E)\in \mathbb {C} } . Here we have:
F A ∧ ω n − 1 = ( F A ⋅ ω ) ω n = λ ( E ) ω n Id . {\displaystyle F_{A}\wedge \omega ^{n-1}=(F_{A}\cdot \omega )\omega ^{n}=\lambda (E)\omega ^{n}\operatorname {Id} .}
Notice that since A {\displaystyle A} is assumed to be a Hermitian connection, the curvature F A {\displaystyle F_{A}} is skew-Hermitian, and so F A 0 , 2 = 0 {\displaystyle F_{A}^{0,2}=0} implies F A 2 , 0 = 0 {\displaystyle F_{A}^{2,0}=0} . When the underlying Kähler manifold X {\displaystyle X} is compact, λ ( E ) {\displaystyle \lambda (E)} may be computed using Chern–Weil theory. Namely, we have
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