Let MM be an oriented without boundary equipped with a , S→MS\to M its , and ∇S\nabla^S its . The spin Dirac operator is the Clifford contraction of the covariant derivative:

D̸=c∘∇S:Γc∞(S)⟶Γc∞(S),D̸ψ=∑j=1dim⁡Mc(ej)∇ejSψ,\not D=c\circ\nabla^S:\Gamma_c^\infty(S)\longrightarrow\Gamma_c^\infty(S),\qquad \not D\psi=\sum_{j=1}^{\dim M}c(e^j)\nabla^S_{e_j}\psi,

where (ej)(e_j) is any local orthonormal frame. The expression is independent of that frame. Its principal symbol is Clifford multiplication, so D̸\not D is a formally self-adjoint .

Analytic realization

With the Riemannian measure and Hermitian spinor metric, D̸\not D is an unbounded on L2(M,S)L^2(M,S). If MM is complete, D̸\not D is , so its closure is self-adjoint. If MM is closed, this realization has compact resolvent and discrete real spectrum of finite multiplicity.

Geometric identities and variants

The Lichnerowicz formula

̸D 2=(∇S)∗∇S+14Scal⁡\not D^{\,2}=(\nabla^S)^*\nabla^S+\frac{1}{4}\operatorname{Scal}

relates the operator to scalar curvature. Twisting SS 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 Z/2\mathbb Z/2-graded and D̸\not D interchanges the two graded pieces.

Conventions and scope

This page is specifically Riemannian: its principal symbol is invertible away from the zero section, so D̸\not D is elliptic, and its analytic realization uses a positive-definite L2L^2 inner product. On a , Clifford contraction instead gives a nonelliptic operator whose characteristic covectors are null. Its flat model is the , and its evolution equation is the . These operators share a Clifford-geometric construction but belong to different analytic categories.

References
  1. 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.
  2. 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.