Definition
Dirac operator
The spin-geometric first-order operator obtained by Clifford contraction of the spin connection.
Let be an oriented Riemannian manifold without boundary equipped with a spin structure, its spinor bundle, and its spin connection. The spin Dirac operator is the Clifford contraction of the covariant derivative:
where is any local orthonormal frame. The expression is independent of that frame. Its principal symbol is Clifford multiplication, so is a formally self-adjoint Dirac-type operator.
Analytic realization
With the Riemannian measure and Hermitian spinor metric, is an unbounded symmetric operator on . If is complete, is essentially self-adjoint, so its closure is self-adjoint. If is closed, this realization has compact resolvent and discrete real spectrum of finite multiplicity.
Geometric identities and variants
The Lichnerowicz formula
relates the operator to scalar curvature. Twisting by a Hermitian bundle with connection yields a twisted Dirac operator with an additional curvature term in its square. In even dimensions the spinor bundle is -graded and interchanges the two graded pieces.
Conventions and scope
This page is specifically Riemannian: its principal symbol is invertible away from the zero section, so is elliptic, and its analytic realization uses a positive-definite inner product. On a Lorentzian spinor bundle, Clifford contraction instead gives a nonelliptic operator whose characteristic covectors are null. Its flat model is the Minkowski Dirac operator, and its evolution equation is the Dirac equation. These operators share a Clifford-geometric construction but belong to different analytic categories.
References
- H. B. Lawson Jr. and M.-L. Michelsohn, Spin Geometry, Princeton University Press, 1989. Publisher record. Relevant: chapter II, §5, spinor bundles and the Dirac operator.
- J. Roe, Elliptic Operators, Topology and Asymptotic Methods, 2nd ed., Chapman & Hall/CRC, 1998. Publisher record. Relevant: chapters 3 and 5, Clifford operators and analytic properties.