Definition

Let (Ai,Hi,Di,Γi)(\mathcal A_i,H_i,D_i,\Gamma_i), i=1,2i=1,2, be over complex . Their product spectral triple has

A=A1A2,H=H1^H2,D=D11+Γ1D2,Γ=Γ1Γ2.\mathcal A=\mathcal A_1\odot\mathcal A_2,\qquad H=H_1\widehat\otimes H_2,\qquad D=\overline{D_1\otimes1+\Gamma_1\otimes D_2}, \qquad \Gamma=\Gamma_1\otimes\Gamma_2.

The algebraic acts on the Hilbert tensor product in the evident way, and the bar denotes the self-adjoint closure from the natural tensor-product core. The grading makes the two unbounded summands anticommute, so D2=D121+1D22D^2=D_1^2\otimes1+1\otimes D_2^2 on that core.

Why the formula works

For aiAia_i\in\mathcal A_i,

[D,a1a2]=[D1,a1]a2+Γ1a1[D2,a2],[D,a_1\otimes a_2] =[D_1,a_1]\otimes a_2 +\Gamma_1a_1\otimes[D_2,a_2],

which is bounded. The anticommutation in the square combines compact resolvents to give for DD under the standard compact spectral-triple hypotheses. These signs are precisely the signs; omitting Γ1\Gamma_1 generally destroys the simple square formula Connes, Part VI.3.

Geometric example

For closed even-dimensional spin manifolds M1M_1 and M2M_2, the product of their canonical spin spectral triples is unitarily equivalent to the canonical triple of M1×M2M_1\times M_2, after the standard identification of product spinors. The displayed Dirac formula becomes the familiar product formula for .

Parity and conventions

If only the first factor is even, the same operator formula defines the even–odd product, which is odd and has no product grading. Odd–odd products require an auxiliary two-dimensional or an equivalent matrix convention. Different choices are unitarily equivalent after the convention is fixed, but writing D11+1D2D_1\otimes1+1\otimes D_2 without a grading sign is not the graded product.

For CC^*-completions of A1A2\mathcal A_1\odot\mathcal A_2, the intended tensor norm must be specified separately; the spectral-triple axioms are imposed on the chosen dense star-subalgebra.

References
  1. Alain Connes, Noncommutative Geometry, Academic Press, 1994. Author-hosted book. Relevant: Part VI.3 on products in spectral geometry.
  2. Walter D. van Suijlekom, Noncommutative Geometry and Particle Physics, Springer, 2015. Publisher record. Relevant: the product construction used in the chapter “Almost-Commutative Manifolds and Gauge Theories,” pp. 137–158.