Definition

An element ee of a JJ is a Jordan idempotent when

ee=e.e\circ e=e.

In a whose product is xy=(xy+yx)/2x\circ y=(xy+yx)/2, this is exactly the usual equation e2=ee^2=e.

Role in the structure theory

Left Jordan multiplication by ee, Le(x)=exL_e(x)=e\circ x, organizes JJ into its . In a unital , idempotents behave like : they can be decomposed into , and maximal compatible decompositions form .

The comparison with projections is exact for . There an element is a Jordan idempotent precisely when it is a self-adjoint projection, and its Jordan rank agrees with the ordinary matrix rank.

References
  1. Kevin McCrimmon, A Taste of Jordan Algebras, Springer, 2004, §§5.1 and 13.1. Publisher record.
  2. Jacques Faraut and Adam Korányi, Analysis on Symmetric Cones, Oxford University Press, 1994, Chapter III. Publisher record.