Jordan Algebras#
- JordanTripleProduct(J): AlgGen -> TenSpcElt#
Returns the tensor describing the Jordan triple product.
- JordanSpinAlgebra(F): TenSpcElt -> AlgGen#
- JordanSpinAlgebra(F): Any -> AlgGen#
Returns the special Jordan algebra of spin type for given symmetric form.
- Example: Ten Jordan Basic (ex-359672)#
Jordan algebras have suggestive analogues of commutative associative algebras, but experimenting shows serious differences.
> F := IdentityMatrix(Rationals(),2); > J := JordanSpinAlgebra(F); > T := Tensor(J); > R := AsMatrices( T, 2,0); > R[1]; // Is J.1 the identity? [1 0 0] [0 1 0] [0 0 1] > J.2*J.2 eq J.1; // J.2^2=1? true > J.2*J.3 eq 0; // Yet J.2 is a zero-divisor. true > e := (1/2)*(J.1+J.2); > e^2 eq e; // An idempotent of J? true
Pierce decompositions in Jordan algebras have the usual 0 and 1 eigenspaces but an additional 1/2-eigenspace emerges as well.
> Re := (1/2)*(R[1]+R[2]); > Eigenvalues(Re); { <1, 1>, <1/2, 1>, <0, 1> }
- ExceptionalJordanCSA(O): AlgGen -> AlgGen#
- ExceptionalJordanCSA(K): Fld -> AlgGen#
The exception central simple Jordan algebra over the given octonions. If a field is supplied instead then the split octonion algebra over the field is used.
- Example: Ten Chevalley Shafer F4 (ex-af7b0b)#
In characteristic not \(2\) or \(3\), the exceptional central simple Jordan algebra can be used to construct the exceptional Lie algebra of type \(F_4\).
> J := ExceptionalJordanCSA(Rationals()); > T := Tensor(J); > T := ChangeTensorCategory(T, HomotopismCategory(3)); > D := DerivationAlgebra(T); > _, D2 := Induce(D, 2); // Represent D on U2. > F4 := D2*D2; // Commutator. > SemisimpleType(F4); F4 > F4; // F4 represented on a 27-dim module. Matrix Lie Algebra of degree 27 over Rational Field