Definition

Let MM be an oriented nn-dimensional without boundary, and let EME\to M be a with and compatible AA. The formal adjoint of the covariant exterior derivative is the operator

dA:Ωr(M;E)Ωr1(M;E)d_A^*:\Omega^{r}(M;E)\longrightarrow\Omega^{r-1}(M;E)

characterized by

dAα,βL2=α,dAβL2\langle d_A\alpha,\beta\rangle_{L^2} =\langle\alpha,d_A^*\beta\rangle_{L^2}

for all compactly supported smooth forms of the appropriate degrees. Here dAd_A is the and the pairing is the . This identity defines a differential expression, not a Hilbert-space adjoint with a specified domain.

Hodge-star formula

Extend the to EE-valued forms by acting on the form factor. With the convention used here, its restriction to rr-forms satisfies

dA=(1)n(r+1)+1dA.d_A^*=(-1)^{n(r+1)+1}*d_A*.

Equivalent sign formulas occur because authors index the input or output degree differently. The compatibility of AA with the fiber metric is what allows without an additional derivative of that metric.

For EE the trivial with its flat connection, dAd_A^* is the ordinary . For the gauge-theoretic adP\operatorname{ad}P, invariance of the Lie-algebra supplies the required bundle metric.

Analytical role

The operator dAd_A^* enters both and the Yang–Mills equation. A perturbation aa is in relative to AA when dAa=0d_A^*a=0, while the is dAFA=0d_A^*F_A=0. Together with dAd_A, it forms the gauge-covariant used in elliptic estimates Freed–Uhlenbeck, chapter 2.

References
  1. Daniel S. Freed and Karen K. Uhlenbeck, Instantons and Four-Manifolds, 2nd ed., Springer, 1991. DOI record. Relevant: chapter 2, bundle-valued forms, formal adjoints, and the Yang–Mills equation.
  2. Raymond O. Wells Jr., Differential Analysis on Complex Manifolds, 3rd ed., Springer, 2008. DOI record. Relevant: chapters III–IV, Hodge-star identities and formal adjoints.