Definition

An even spectral triple is a (A,H,D)(\mathcal A,H,D) together with a operator Γ\Gamma on HH such that

Γ=Γ,Γ2=1,Γa=aΓ,ΓD=DΓ\Gamma=\Gamma^*,\qquad \Gamma^2=1,\qquad \Gamma a=a\Gamma,\qquad \Gamma D=-D\Gamma

for every aAa\in\mathcal A, with ΓDom(D)=Dom(D)\Gamma\operatorname{Dom}(D)=\operatorname{Dom}(D). Thus the algebra representation is even and DD is an in the unbounded, domain-sensitive sense. Equivalently, H=H+HH=H^+\oplus H^-, every aa preserves the two summands, and DD interchanges them.

Block form

Relative to H+HH^+\oplus H^-, the data have the form

a=(a+00a),D=(0DD+0),a= \begin{pmatrix} a^+&0\\ 0&a^- \end{pmatrix}, \qquad D= \begin{pmatrix} 0&D^-\\ D^+&0 \end{pmatrix},

where self-adjointness gives D=(D+)D^-=(D^+)^*, with the corresponding domains understood. The off-diagonal form is precisely the anticommutation relation ΓD=DΓ\Gamma D=-D\Gamma.

Geometric example

On a closed even-dimensional Riemannian spin manifold, the complex splits as

S=S+S.S=S^+\oplus S^-.

The chirality operator supplies Γ\Gamma, functions preserve the splitting, and the spin exchanges positive and negative spinors. The canonical spectral triple is therefore even.

Index pairing

For a projection pp over the algebra, the represented projection preserves the graded subspaces. Under the usual compactness hypotheses, the compression of the positive part,

pD+p:pH+pH,pD^+p:pH^+\longrightarrow pH^-,

has a Fredholm realization, and its integer index gives the even pairing with K-theory. Precise domain and matrix-amplification conventions are part of the pairing construction, not extra axioms in the definition above.

Graded-algebra variant

The standard definition assumes that A\mathcal A is trivially graded, which is why every represented aa commutes with Γ\Gamma. If A\mathcal A itself is graded, a graded representation and graded commutators replace these ordinary parity relations. That convention is broader and should be stated explicitly.

References