Definition

Let JJ be a . Its Jordan trace form is

τ(x,y)=trJ(xy),\tau(x,y)=\operatorname{tr}_J(x\circ y),

where trJ(x)\operatorname{tr}_J(x) is the sum of the Jordan eigenvalues of xx.

Fundamental properties

The form τ\tau is symmetric, positive definite, and associative:

τ(xy,z)=τ(x,yz).\tau(x\circ y,z)=\tau(x,y\circ z).

Thus it is a canonical compatible Euclidean . A Euclidean Jordan algebra may be presented with another compatible inner product; on each simple ideal, every such form is a positive scalar multiple of the canonical trace form. Different simple summands may carry different positive scalings.

Matrix and spin-factor cases

On hn(R)\mathfrak h_n(\mathbb R), hn(C)\mathfrak h_n(\mathbb C), and hn(H)\mathfrak h_n(\mathbb H), the Jordan trace is the ordinary real matrix trace, and

τ(X,Y)=ReTr(XY).\tau(X,Y)=\operatorname{Re}\operatorname{Tr}(XY).

For J(V)=RVJ(V)=\mathbb R\oplus V,

trJ(λ,u)=2λ,τ((λ,u),(μ,v))=2(λμ+u,v).\operatorname{tr}_J(\lambda,u)=2\lambda,\qquad \tau((\lambda,u),(\mu,v)) =2(\lambda\mu+\langle u,v\rangle).
Operator-trace convention

Another , also sometimes called “the trace form,” is

β(x,y)=Tr(Lxy),Lx(z)=xz.\beta(x,y)=\operatorname{Tr}(L_{x\circ y}), \qquad L_x(z)=x\circ z.

Here Tr\operatorname{Tr} is the trace of a vector-space endomorphism. On a of dimension NN and rank rr,

β(x,y)=Nrτ(x,y).\beta(x,y)=\frac Nr\,\tau(x,y).

The conventions differ only by a positive factor on each simple ideal, but a formula should identify its normalization.

Every Jordan automorphism preserves spectral eigenvalues and hence trJ\operatorname{tr}_J and τ\tau. This realizes Aut(J)\operatorname{Aut}(J) as a closed subgroup of the of the trace form.

References
  1. Jacques Faraut and Adam Korányi, Analysis on Symmetric Cones, Oxford University Press, 1994. Publisher record.
  2. Tonny A. Springer and Ferdinand D. Veldkamp, Octonions, Jordan Algebras and Exceptional Groups, Springer, 2000. Publisher record.