Definition

Let (M,g)(M,g) be an oriented nn-dimensional . The metric and determine an on kk-forms and a volume form volg\operatorname{vol}_g. The Hodge star operator is the unique linear isomorphism

:Ωk(M)Ωnk(M)*:\Omega^k(M)\longrightarrow\Omega^{n-k}(M)

such that, for all real kk-forms α,β\alpha,\beta,

αβ=α,βgvolg.\alpha\wedge *\beta=\langle\alpha,\beta\rangle_g\,\operatorname{vol}_g.

It is defined pointwise and varies smoothly with gg. Thus the star combines the , the metric, and orientation into an operator complementary in degree.

Characterizing identities

On real kk-forms in the Riemannian convention,

(α)=(1)k(nk)α.*(*\alpha)=(-1)^{k(n-k)}\alpha.

The star is a pointwise isometry, and 1=volg*1=\operatorname{vol}_g, while volg=1*\operatorname{vol}_g=1. These identities follow directly in an oriented orthonormal coframe and characterize the signs used here. The construction and its role in the Laplacian are treated in Morita, “Laplacian and harmonic forms”.

The star also converts the into its , up to a degree- and dimension-dependent sign. This is the basic mechanism behind the and harmonic-form theory.

Computation in an orthonormal coframe

If e1,,ene^1,\ldots,e^n is a positively oriented orthonormal coframe and I=(i1<<ik)I=(i_1<\cdots<i_k), then eI*e^I is the uniquely signed complementary wedge eIce^{I^c} for which

eIeI=e1en.e^I\wedge *e^I=e^1\wedge\cdots\wedge e^n.

For the standard orientation of R3\mathbb R^3, for example, dx=dydz*dx=dy\wedge dz, dy=dzdx*dy=dz\wedge dx, and dz=dxdy*dz=dx\wedge dy.

Conventions and scope
References
  1. Shigeyuki Morita, Geometry of Differential Forms, Translations of Mathematical Monographs 201, American Mathematical Society, 2001. Publisher record. Relevant: “Laplacian and harmonic forms.”
  2. Raymond O. Wells Jr., Differential Analysis on Complex Manifolds, 3rd ed., Graduate Texts in Mathematics 65, Springer, 2008. Publisher record. Relevant: Chapter III, “Differential Geometry,” Hermitian exterior algebra and the Hodge star.