In mathematics, symmetric cones, sometimes called domains of positivity, are open convex self-dual cones in Euclidean space which have a transitive group of symmetries, i.e. invertible operators that take the cone onto itself. By the Koecher–Vinberg theorem these correspond to the cone of squares in finite-dimensional real Euclidean Jordan algebras, originally studied and classified by . The tube domain associated with a symmetric cone is a noncompact Hermitian symmetric space of tube type. All the algebraic and geometric structures associated with the symmetric space can be expressed naturally in terms of the Jordan algebra. The other irreducible Hermitian symmetric spaces of noncompact type correspond to Siegel domains of the second kind. These can be described in terms of more complicated structures called Jordan triple systems, which generalize Jordan algebras without identity.[1]
A convex cone C in a finite-dimensional real inner product space V is a convex set invariant under multiplication by positive scalars. It spans the subspace C – C and the largest subspace it contains is C ∩ (−C). It spans the whole space if and only if it contains a basis. Since the convex hull of the basis is a polytope with non-empty interior, this happens if and only if C has non-empty interior. The interior in this case is also a convex cone. Moreover, an open convex cone coincides with the interior of its closure, since any interior point in the closure must lie in the interior of some polytope in the original cone. A convex cone is said to be proper if its closure, also a cone, contains no subspaces.
Let C be an open convex cone. Its dual is defined as
\displaystyle{C*=\{X:(X,Y)>0forY\in\overline{C}\}.}
It is also an open convex cone and C** = C. An open convex cone C is said to be self-dual if C* = C. It is necessarily proper, sinceit does not contain 0, so cannot contain both X and −X.
The automorphism group of an open convex cone is defined by
\displaystyle{AutC=\{g\inGL(V)|gC=C\}.}
Clearly g lies in Aut C if and only if g takes the closure of C onto itself. So Aut C is a closed subgroup of GL(V) and hence a Lie group. Moreover, Aut C* = (Aut C)*, where g* is the adjoint of g. C is said to be homogeneous if Aut C acts transitively on C.
The open convex cone C is called a symmetric cone if it is self-dual and homogeneous.
In their classic paper, studied and completely classified a class of finite-dimensional Jordan algebras, that are now called either Euclidean Jordan algebras or formally real Jordan algebras.
Let E be a finite-dimensional real vector space with a symmetric bilinear product operation
\displaystyle{E x E → E,a,b\mapstoab=ba,}
with an identity element 1 such that a1 = a for a in A and a real inner product (a,b) for which the multiplication operators L(a) defined by L(a)b = ab on E are self-adjoint and satisfy the Jordan relation
\displaystyle{L(a)L(a2)=L(a2)L(a).}
As will turn out below, the condition on adjoints can be replaced by the equivalent condition thatthe trace form Tr L(ab) defines an inner product. The trace form has the advantage of being manifestly invariant under automorphisms of the Jordan algebra, which is thus a closed subgroup of O(E) and thus a compact Lie group. In practical examples, however, it is often easier to produce an inner product for which the L(a) are self-adjoint than verify directly positive-definiteness of the trace form. (The equivalent original condition of Jordan, von Neumann and Wigner was that if a sum of squares of elements vanishes then each of those elements has to vanish.[2])
From the Jordan condition it follows that the Jordan algebra is power associative, i.e. the Jordan subalgebra generated by any single element a in E is actually an associative commutative algebra. Thus, defining an inductively by an = a (an−1), the following associativity relation holds:
\displaystyle{aman=am+n,}
so the subalgebra can be identified with R[''a''], polynomials in a. In fact polarizing of the Jordan relation—replacing a by a + tb and taking the coefficient of t—yields
\displaystyle{2L(ab)L(a)+L(a2)L(b)=2L(a)L(b)L(a)+L(a2b).}
This identity implies that L(am) is a polynomial in L(a) and L(a2) for all m. In fact, assuming the result for lower exponents than m,
\displaystyle{a2am-1=am-1(a2)=L(am-1)L(a)a=L(a)L(am-1)a=L(a)am=am+1.}
Setting b = am – 1 in the polarized Jordan identity gives:
\displaystyle{L(am+1)=2L(am)L(a)+L(a2)L(am-1)-2L(a)2L(am-1),}
a recurrence relation showing inductively that L(am + 1) is a polynomial in L(a) and L(a2).
Consequently, if power-associativity holds when the first exponent is ≤ m, then it also holds for m+1 since
\displaystyle{L(am+1)an=2L(a)L(am)an+L(a2)L(am-1)an-2L(a)2L(am-1)an =am+n+1.}
An element e in E is called an idempotent if e2 = e. Two idempotents are said to be orthogonal if ef = 0. This is equivalent to orthogonality with respect to the inner product, since (ef,ef) = (e,f). In this case g = e + f is also an idempotent. An idempotent g is called primitive or minimal if it cannot be written as a sum of non-zero orthogonal idempotents. If e1, ..., em are pairwise orthogonal idempotents then their sum is also an idempotent and the algebra they generate consists of all linear combinations of the ei. It is an associative algebra. If e is an idempotent, then 1 − e is an orthogonal idempotent. An orthogonal set of idempotents with sum 1 is said to be a complete set or a partition of 1. If each idempotent in the set is minimal it is called a Jordan frame. Since the number of elements in any orthogonal set of idempotents is bounded by dim E, Jordan frames exist. The maximal number of elements in a Jordan frame is called the rank r of E.
The spectral theorem states that any element a can be uniquely written as
\displaystyle{a=\sumλiei,}
where the idempotents ei's are a partition of 1 and the λi, the eigenvalues of a, are real and distinct. In fact let E0 = R[a] and let T be the restriction of L(a) to E0. T is self-adjoint and has 1 as a cyclic vector. So the commutant of T consists of polynomials in T (or a). By the spectral theorem for self-adjoint operators,
\displaystyle{T=\sumλiPi}
where the Pi are orthogonal projections on E0 with sum I and the λi's are the distinct real eigenvalues of T. Since the Pi's commute with T and are self-adjoint, they are given by multiplication elements ei of R[a] and thus form a partition of 1. Uniqueness follows because if fi is a partition of 1 and a = Σ μi fi, then with p(t)=Π (t - μj) and pi = p/(t − μi), fi = pi(a)/pi(μi). So the fi's are polynomials in a and uniqueness follows from uniqueness of the spectral decomposition of T.
The spectral theorem implies that the rank is independent of the Jordan frame. For a Jordan frame with k minimal idempotents can be used to construct an element a with k distinct eigenvalues. As above the minimal polynomial p of a has degree k and R[''a''] has dimension k. Its dimension is also the largest k such that Fk(a) ≠ 0 where Fk(a) is the determinant of a Gram matrix:
\displaystyle{Fk(a)=\det0\le(am,an).}
So the rank r is the largest integer k for which Fk is not identically zero on E. In this case, as a non-vanishing polynomial, Fr is non-zero on an open dense subset of E. the regular elements. Any other a is a limit of regular elements a(n). Since the operator norm of L(x) gives an equivalent norm on E, a standard compactness argument shows that, passing to a subsequence if necessary, the spectral idempotents of the a(n) and their corresponding eigenvalues are convergent. The limit of Jordan frames is a Jordan frame, since a limit of non-zero idempotents yields a non-zero idempotent by continuity of the operator norm. It follows that every Jordan frame is made up of r minimal idempotents.
If e and f are orthogonal idempotents, the spectral theorem shows that e and f are polynomials in a = e − f, so that L(e) and L(f) commute. This can be seen directly from the polarized Jordan identity which implies L(e)L(f) = 2 L(e)L(f)L(e). Commutativity follows by taking adjoints.
If e is a non-zero idempotent then the eigenvalues of L(e) can only be 0, 1/2 and 1, since taking a = b = e in the polarized Jordan identity yields
\displaystyle{2L(e)3-3L(e)2+L(e)=0.}
In particular the operator norm of L(e) is 1 and its trace is strictly positive.
There is a corresponding orthogonal eigenspace decomposition of E
\displaystyle{E=E0(e) ⊕ E1/2(e) ⊕ E1(e),}
where, for a in E, Eλ(a) denotes the λ-eigenspace of L(a). In this decomposition E1(e) and E0(e) are Jordan algebras with identity elements e and 1 − e. Their sum E1(e) ⊕ E0(e) is a direct sum of Jordan algebras in that any product between them is zero. It is the centralizer subalgebra of e and consists of all a such that L(a) commutes with L(e). The subspace E1/2(e) is a module for the centralizer of e, the centralizer module, and the product of any two elements in it lies in the centralizer subalgebra. On the other hand, if
\displaystyle{U=8L(e)2-8L(e)+I,}
then U is self-adjoint equal to 1 on the centralizer algebra and −1 on the centralizer module. So U2 = I and the properties above show that
\displaystyle{\sigma(x)=Ux}
defines an involutive Jordan algebra automorphism σ of E.
In fact the Jordan algebra and module properties follow by replacing a and b in the polarized Jordan identity by e and a. If ea = 0, this gives L(e)L(a) = 2L(e)L(a)L(e). Taking adjoints it follows that L(a) commutes with L(e). Similarly if (1 − e)a = 0, L(a) commutes with I − L(e) and hence L(e). This implies the Jordan algebra and module properties. To check that a product of elements in the module lies in the algebra, it is enough to check this for squares: but if L(e)a = a, then ea = a, so L(a)2 + L(a2)L(e) = 2L(a)L(e)L(a) + L(a2e). Taking adjoints it follows that L(a2) commutes with L(e), which implies the property for squares.
The trace form is defined by
\displaystyle{\tau(a,b)=TrL(ab).}
It is an inner product since, for non-zero a = Σ λi ei,
\displaystyle{\tau(a,a)=\sum
| 2 | |
| λ | |
| i |
TrL(ei)>0.}
The polarized Jordan identity can be polarized again by replacing a by a + tc and taking the coefficient of t. A further anyisymmetrization in a and c yields:
\displaystyle{L(a(bc)-(ab)c)=[[L(a),L(b)],L(c)].}
Applying the trace to both sides
\displaystyle{\tau(a,bc)=\tau(ba,c),}
so that L(b) is self-adjoint for the trace form.
The classification of simple Euclidean Jordan algebras was accomplished by, with details of the one exceptional algebra provided in the article immediately following theirs by . Using the Peirce decomposition, they reduced the problem to an algebraic problem involving multiplicative quadratic forms already solved by Hurwitz. The presentation here, following, using composition algebras or Euclidean Hurwitz algebras, is a shorter version of the original derivation.
If E is a Euclidean Jordan algebra an ideal F in E is a linear subspace closed under multiplication by elements of E, i.e. F is invariant under the operators L(a) for a in E. If P is the orthogonal projection onto F it commutes with the operators L(a), In particular F⊥ = (I − P)E is also an ideal and E = F ⊕ F⊥. Furthermore, if e = P(1), then P = L(e). In fact for a in E
\displaystyle{ea=ae=L(a)P(1)=P(L(a)1)=P(a),}
so that ea = a for a in F and 0 for a in F⊥. In particular e and 1 − e are orthogonal idempotents with L(e) = P and L(1 − e) = I − P. e and 1 − e are the identities in the Euclidean Jordan algebras F and F⊥. The idempotent e is central in E, where the center of E is defined to be the set of all z such that L(z) commutes with L(a) for all a. It forms a commutative associative subalgebra.
Continuing in this way E can be written as a direct sum of minimal ideals
\displaystyle{E= ⊕ Ei.}
If Pi is the projection onto Ei and ei = Pi(1) then Pi = L(ei). The ei's are orthogonal with sum 1 and are the identities in Ei. Minimality forces Ei to be simple, i.e. to have no non-trivial ideals. For since L(ei) commutes with all L(a)'s, any ideal F ⊂ Eiwould be invariant under E since F = eiF. Such a decomposition into a direct sum of simple Euclidean algebras is unique. If E = ⊕ Fj is another decomposition, then Fj=⊕ eiFj. By minimality only one of the terms here is non-zero so equals Fj. By minimality the corresponding Ei equals Fj, proving uniqueness.
In this way the classification of Euclidean Jordan algebras is reduced to that of simple ones. For a simple algebra E all inner products for which the operators L(a) are self adjoint are proportional. Indeed, any other product has the form (Ta, b) for some positive self-adjoint operator commuting with the L(a)'s. Any non-zero eigenspace of T is an ideal in A and therefore by simplicity T must act on the whole of E as a positive scalar.
The Jordan algebras H2(R), H2(C), H2(H) and H2(O) are isomorphic to spin factors V ⊕ R where V has dimension 2, 3, 5 and 9, respectively: that is, one more than the dimension of the relevant division algebra.
See also: Peirce decomposition. Let E be a simple Euclidean Jordan algebra with inner product given by the trace form τ(a)= Tr L(a). The proof that E has the above form rests on constructing an analogue of matrix units for a Jordan frame in E. The following properties of idempotents hold in E.
See main article: article and Euclidean Hurwitz algebra. Let E be a simple Euclidean Jordan algebra. From the properties of the Peirce decomposition it follows that:
Such an algebra A is called a Euclidean Hurwitz algebra. In A if λ(a)b = ab and ρ(a)b = ba, then:
By Hurwitz's theorem A must be isomorphic to R, C, H or O. The first three are associative division algebras. The octonions do not form an associative algebra, so Hr(O) can only give a Jordan algebra for r = 3. Because A is associative when A = R, C or H, it is immediate that Hr(A) is a Jordan algebra for r ≥ 3. A separate argument, given originally by, is required to show that H3(O) with Jordan product a∘b = (ab + ba) satisfies the Jordan identity [''L''(''a''),''L''(''a''<sup>2</sup>)] = 0. There is a later more direct proof using the Freudenthal diagonalization theorem due to : he proved that given any matrix in the algebra Hr(A) there is an algebra automorphism carrying the matrix onto a diagonal matrix with real entries; it is then straightforward to check that [''L''(''a''),''L''(''b'')] = 0 for real diagonal matrices.[3]
The exceptional Euclidean Jordan algebra E= H3(O) is called the Albert algebra. The Cohn–Shirshov theorem implies that it cannot be generated by two elements (and the identity). This can be seen directly. For by Freudenthal's diagonalization theorem one element X can be taken to be a diagonal matrix with real entries and the other Y to be orthogonal to the Jordan subalgebra generated by X. If all the diagonal entries of X are distinct, the Jordan subalgebra generated by X and Y is generated by the diagonal matrices and three elements
\displaystyle{Y1=\begin{pmatrix}0&0&0\ 0&0&y1\\0&
| * | |
| y | |
| 1 |
&0\end{pmatrix}, Y2=\begin{pmatrix}0&0&
| *\ 0 | |
| y | |
| 2 |
&0&0\\y2&0&0\end{pmatrix}, Y3=\begin{pmatrix}0&y3&
| * | |
| 0\ y | |
| 3 |
&0&0\\0&0&0\end{pmatrix}.}
It is straightforward to verify that the real linear span of the diagonal matrices, these matrices and similar matrices with real entries form a unital Jordan subalgebra. If the diagonal entries of X are not distinct, X can be taken to be the primitive idempotent e1 with diagonal entries 1, 0 and 0. The analysis in then shows that the unital Jordan subalgebra generated by X and Y is proper. Indeed, if 1 − e1 is the sum of two primitive idempotents in the subalgebra, then, after applying an automorphism of E if necessary, the subalgebra will be generated by the diagonal matrices and a matrix orthogonal to the diagonal matrices. By the previous argument it will be proper. If 1 - e1 is a primitive idempotent, the subalgebra must be proper, by the properties of the rank in E.
A Euclidean algebra is said to be special if its central decomposition contains no copies of the Albert algebra. Since the Albert algebra cannot be generated by two elements, it follows that a Euclidean Jordan algebra generated by two elements is special. This is the Shirshov–Cohn theorem for Euclidean Jordan algebras.[4]
The classification shows that each non-exceptional simple Euclidean Jordan algebra is a subalgebra of some Hn(R). The same is therefore true of any special algebra.
On the other hand, as showed, the Albert algebra H3(O) cannot be realized as a subalgebra of Hn(R) for any n.[5]
Indeed, let π is a real-linear map of E = H3(O) into the self-adjoint operators on V = Rn with π(ab) = (π(a)π(b) + π(b)π(a)) and π(1) = I. If e1, e2, e3 are the diagonal minimal idempotents then Pi = π(ei are mutually orthogonal projections on V onto orthogonal subspaces Vi. If i ≠ j, the elements eij of E with 1 in the (i,j) and (j,i) entries and 0 elsewhere satisfy eij2 = ei + ej. Moreover, eijejk = eik if i, j and k are distinct. The operators Tij are zero on Vk (k ≠ i, j) and restrict to involutions on Vi ⊕ Vj interchanging Vi and Vj. Letting Pij = Pi Tij Pj and setting Pii = Pi, the (Pij) form a system of matrix units on V, i.e. Pij* = Pji, Σ Pii = I and PijPkm = δjk Pim. Let Ei and Eij be the subspaces of the Peirce decomposition of E. For x in O, set πij = Pij π(xeij), regarded as an operator on Vi. This does not depend on j and for x, y in O
\displaystyle{\piij(xy)=\piij(x)\piij(y),\piij(1)=I.}
Since every x in O has a right inverse y with xy = 1, the map πij is injective. On the other hand, it is an algebra homomorphism from the nonassociative algebra O into the associative algebra End Vi, a contradiction.
When (ei) is a partition of 1 in a Euclidean Jordan algebra E, the self-adjoint operators L(ei) commute and there is a decomposition into simultaneous eigenspaces. If a = Σ λi ei the eigenvalues of L(a) have the form Σ εi λi is 0, 1/2 or 1. The ei themselves give the eigenvalues λi. In particular an element a has non-negative spectrum if and only if L(a) has non-negative spectrum. Moreover, a has positive spectrum if and only if L(a) has positive spectrum. For if a has positive spectrum, a - ε1 has non-negative spectrum for some ε > 0.
The positive cone C in E is defined to be the set of elements a such that a has positive spectrum. This condition is equivalent to the operator L(a) being a positive self-adjoint operator on E.
To show that the positive cone C is homogeneous, i.e. has a transitive group of automorphisms, a generalization of the quadratic action of self-adjoint matrices on themselves given by X ↦ YXY has to be defined. If Y is invertible and self-adjoint, this map is invertible and carries positive operators onto positive operators.
For a in E, define an endomorphism of E, called the quadratic representation, by
\displaystyle{Q(a)=2L(a)2-L\left(a2\right).}
Note that for self-adjoint matrices L(X)Y = (XY + YX), so that Q(X)Y = XYX.
An element a in E is called invertible if it is invertible in R[''a'']. If b denotes the inverse, then the spectral decomposition of a shows that L(a) and L(b) commute.
In fact a is invertible if and only if Q(a) is invertible. In that case
Indeed, if Q(a) is invertible it carries R[''a''] onto itself. On the other hand, Q(a)1 = a2, so
\displaystyle{\left(Q(a)-1a\right)a=aQ(a)-1a=L(a)Q(a)-1a=Q(a)-1a2=1.}
Taking b = a−1 in the polarized Jordan identity, yields
\displaystyle{Q(a)L\left(a-1\right)=L(a).}
Replacing a by its inverse, the relation follows if L(a) and L(a−1) are invertible. If not it holds for a + ε1 with ε arbitrarily small and hence also in the limit.
These identities are easy to prove in a finite-dimensional (Euclidean) Jordan algebra (see below) or in a special Jordan algebra, i.e. the Jordan algebra defined by a unital associative algebra.[6] They are valid in any Jordan algebra. This was conjectured by Jacobson and proved in : Macdonald showed that if a polynomial identity in three variables, linear in the third, is valid in any special Jordan algebra, then it holds in all Jordan algebras.[7]
In fact for c in A and F(a) a function on A with values in End A, letDcF(a) be the derivative at t = 0 of F(a + tc). Then
\displaystyle{c=
| -1 | |
| D | |
| c\left(Q(a)a |
\right)=2\left[(L(a)L(c)+L(c)L(a)-L(ac))a-1\right]+
| -1 | |
| Q(a)D | |
| c\left(a |
\right)=2c+
| -1 | |
| Q(a)D | |
| c\left(a |
\right).}
The expression in square brackets simplifies to c because L(a) commutes with L(a−1).
Thus
Applying Dc to L(a−1)Q(a) = L(a) and acting on b = c−1 yields
\displaystyle{(Q(a)b)\left(Q\left(a-1\right)b-1\right)=1.}
On the other hand, L(Q(a)b) is invertible on an open dense set where Q(a)b must also be invertible with
\displaystyle{(Q(a)b)-1=Q\left(a-1\right)b-1.}
Taking the derivative Dc in the variable b in the expression above gives
\displaystyle{-Q(Q(a)b)-1Q(a)c=-Q(a)-1Q(b)-1c.}
This yields the fundamental identity for a dense set of invertible elements, so it follows in general by continuity. The fundamental identity implies that c = Q(a)b is invertible if a and b are invertible and gives a formula for the inverse of Q(c). Applying it to c gives the inverse identity in full generality.
Finally it can be verified immediately from the definitions that, if u = 1 − 2e for some idempotent e, then Q(u) is the period 2 automorphism constructed above for the centralizer algebra and module of e.
The proof of this relies on elementary continuity properties of eigenvalues of self-adjoint operators.[8]
Let T(t) (α ≤ t ≤ β) be a continuous family of self-adjoint operators on E with T(α) positive and T(β) having a negative eigenvalue. Set S(t)= –T(t) + M with M > 0 chosen so large that S(t) is positive for all t. The operator norm ||S(t)|| is continuous. It is less than M for t = α and greater than M for t = β. So for some α < s < β, ||S(s)|| = M and there is a vector v ≠ 0 such that S(s)v = Mv. In particular T(s)v = 0, so that T(s) is not invertible.
Suppose that x = Q(a)b does not lie in C. Let b(t) = (1 − t) + tb with 0 ≤ t ≤ 1. By convexity b(t) lies in C. Let x(t) = Q(a)b(t) and X(t) = L(x(t)). If X(t) is invertible for all t with 0 ≤ t ≤ 1, the eigenvalue argument gives a contradiction since it is positive at t = 0 and has negative eigenvalues at t = 1. So X(s) has a zero eigenvalue for some s with 0 < s ≤ 1: X(s)w = 0 with w ≠ 0. By the properties of the quadratic representation, x(t) is invertible for all t. Let Y(t) = L(x(t)2). This is a positive operator since x(t)2 lies in C. Let T(t) = Q(x(t)), an invertible self-adjoint operator by the invertibility of x(t). On the other hand, T(t) = 2X(t)2 - Y(t). So (T(s)w,w) < 0 since Y(s) is positive and X(s)w = 0. In particular T(s) has some negative eigenvalues. On the other hand, the operator T(0) = Q(a2) = Q(a)2 is positive. By the eigenvalue argument, T(t) has eigenvalue 0 for some t with 0 < t < s, a contradiction.
It follows that the linear operators Q(a) with a invertible, and their inverses, take the cone C onto itself. Indeed, the inverse of Q(a) is just Q(a−1). Since Q(a)1 = a2, there is thus a transitive group of symmetries:
Let C be a symmetric cone in the Euclidean space E. As above, Aut C denotes the closed subgroup of GL(E) taking C (or equivalently its closure) onto itself. Let G = Aut0 C be its identity component. K = G ∩ O(E). It is a maximal compact subgroup of G and the stabilizer of a point e in C. It is connected. The group G is invariant under taking adjoints. Let σg =(g*)−1, period 2 automorphism. Thus K is the fixed point subgroup of σ. Let
ak{g}
ak{g}
\displaystyle{ak{g}=ak{k} ⊕ ak{p},}
where
ak{k}
ak{p}
ak{p}
ak{p}
ak{p}
ak{p}
ak{p}
Since the elements of
ak{p}
ak{k}
The associator is given by [''a'',''b'',''c''] = [''L''(''a''),''L''(''c'')]b. Since [''L''(''a''),''L''(''c'')] lies in
ak{k}
\displaystyle{[a,b2,c]=2[a,b,c]b.}
On the other hand,
\displaystyle{([b2,a,b],c)=(b2(ba)-b(b2a),c)=-(b2,[a,b,c])}
and likewise
\displaystyle{([b2,a,b],c)=(b,[a,b2,c]).}
Combining these expressions gives
\displaystyle{([b2,a,b],c)=0,}
which implies the Jordan identity.
Finally the positive cone of E coincides with C. This depends on the fact that in any Euclidean Jordan algebra E
\displaystyle{Q(ea)=e2L(a).}
In fact Q(ea) is a positive operator,Q(eta) is a one-parameter group of positive operators: this follows by continuity for rational t, where it is a consequence of the behaviour of powers So it has the form exp tX for some self-adjoint operator X. Taking the derivative at 0 gives X = 2L(a).
Hence the positive cone is given by all elements
\displaystyle{e2a=Q(ea)1=e2L(a)1=eX ⋅ 1,}
with X in
ak{p}
Let C be the positive cone in a simple Euclidean Jordan algebra E. Aut C is the closed subgroup of GL(E) taking C (or its closure) onto itself. Let G = Aut0 C be the identity component of Aut C and let K be the closed subgroup of G fixing 1. From the group theoretic properties of cones, K is a connected compact subgroup of G and equals the identity component of the compact Lie group Aut E. Let
ak{g}
ak{k}
ak{p}
ak{k}
ak{k}
ak{k}
ak{p}
ak{a}
ak{p}
ak{p}
ak{a}
ak{p}
ak{a}
If E has Peirce decomposition relative to the Jordan frame (ei)
\displaystyle{E=oplusi\leEij,}
then
ak{a}
Define the closed subgroup S of G by
\displaystyle{S=\{g\inG|gEij\subseteqoplus(p,q)\geEpq\},}
where the ordering on pairs p ≤ q is lexicographic. S contains the group A, since it acts as scalars on Eij. If N is the closed subgroup of S such that nx = x modulo ⊕(p,q) > (i,j) Epq, then S = AN = NA, a semidirect product with A normalizing N. Moreover, G has the following Iwasawa decomposition:
\displaystyle{G=KAN.}
For i ≠ j let
\displaystyle{ak{g}ij=\{X\inak{g}:[L(a),X]={1\over2}(\alphai-\alphaj)X,fora=\sum\alphaiei\}.}
Then the Lie algebra of N is
\displaystyle{ak{n}=oplusi<jak{g}ij,ak{g}ij=\{L(a)+2[L(a),L(ei)]:a\inEij\}.}
Taking ordered orthonormal bases of the Eij gives a basis of E, using the lexicographic order on pairs (i,j). The group N is lower unitriangular and its Lie algebra lower triangular. In particular the exponential map is a polynomial mapping of
ak{n}
Let E be a Euclidean Jordan algebra. The complexification EC = E ⊕ iE has a natural conjugation operation (a + ib)* = a − ib and a natural complex inner product and norm. The Jordan product on E extends bilinearly to EC, so that (a + ib)(c + id) = (ac − bd) + i(ad + bc). If multiplication is defined by L(a)b = ab then the Jordan axiom
\displaystyle{[L(a),L(a2)]=0}
still holds by analytic continuation. Indeed, the identity above holds when a is replaced by a + tb for t real; and since the left side is then a polynomial with values in End EC vanishing for real t, it vanishes also t complex. Analytic continuation also shows that all for the formulas involving power-associativity for a single element a in E, including recursion formulas for L(am), also hold in EC. Since for b in E, L(b) is still self-adjoint on EC, the adjoint relation L(a*) = L(a)* holds for a in EC. Similarly the symmetric bilinear form β(a,b) = (a,b*) satisfies β(ab,c) = β(b,ac). If the inner product comes from the trace form, then β(a,b) = Tr L(ab).
For a in EC, the quadratic representation is defined as before by Q(a)=2L(a)2 − L(a2). By analytic continuation the fundamental identity still holds:
\displaystyle{Q(Q(a)b)=Q(a)Q(b)Q(a),Q(am)=Q(a)m(m\ge0).}
An element a in E is called invertible if it is invertible in C[''a'']. Power associativity shows that L(a) and L(a−1) commute. Moreover, a−1 is invertible with inverse a.
As in E, a is invertible if and only if Q(a) is invertible. In that case
\displaystyle{Q(a)-1a=a-1,Q(a-1)=Q(a)-1.}
Indeed, as for E, if Q(a) is invertible it carries C[''a''] onto itself, while Q(a)1 = a2, so
\displaystyle{(Q(a)-1a)a=aQ(a)-1a=L(a)Q(a)-1a=Q(a)-1a2=1,}
so a is invertible. Conversely if a is invertible, taking b = a−2 in the fundamental identity shows that Q(a) is invertible. Replacing a by a−1 and b by a then shows that its inverse is Q(a−1). Finally if a and b are invertible then so is c = Q(a)b and it satisfies the inverse identity:
\displaystyle{(Q(a)b)-1=Q(a-1)b-1.}
Invertibility of c follows from the fundamental formula which gives Q(c) = Q(a)Q(b)Q(a). Hence
\displaystyle{c-1=Q(c)-1c=Q(a)-1Q(b)-1b=Q(a)-1b-1.}
The formula
\displaystyle{Q(ea)=e2L(a)
also follows by analytic continuation.
Aut EC is the complexification of the compact Lie group Aut E in GL(EC). This follows because the Lie algebras of Aut EC and Aut E consist of derivations of the complex and real Jordan algebras EC and E. Under the isomorphism identifying End EC with the complexification of End E, the complex derivations is identified with the complexification of the real derivations.
The Jordan operator L(a) are symmetric with respect to the trace form, so that L(a)t = L(a) for a in EC. The automorphism groups of E and EC consist of invertible real and complex linear operators g such that L(ga) = gL(a)g−1 and g1 = 1. Aut EC is the complexification of Aut E. Since an automorphism g preserves the trace form, g−1 = gt.
The structure groups of E and EC consist of invertible real and complex linear operators g such that
\displaystyle{Q(ga)=gQ(a)gt.}
They form groups Γ(E) and Γ(EC) with Γ(E) ⊂ Γ(EC).
ak{k} ⊕ ak{p}
The unitary structure group Γu(EC) is the subgroup of Γ(EC) consisting of unitary operators, so that Γu(EC) = Γ(EC) ∩ U(EC).
ak{k} ⊕ iak{p}
Given a frame in a Euclidean Jordan algebra E, the restricted Weyl group can be identified with the group of operators on arising from elements in the identity component of Γu(EC) that leave invariant.
Let E be a Euclidean Jordan algebra with the inner product given by the trace form. Let (ei) be a fixed Jordan frame in E. For given a in EC choose u in Γu(EC) such thatua = Σ αi ei with αi ≥ 0. Then the spectral norm ||a|| = max αi is independent of all choices. It is a norm on EC with
\displaystyle{\|a*\|=\|a\|,\|\{a,a*,a\}\|=\|a\|3.}
In addition ||a||2 is given by the operator norm of Q(a) on the inner product space EC. The fundamental identity for the quadratic representation implies that ||Q(a)b|| ≤ ||a||2||b||. The spectral norm of an element a is defined in terms of C[''a''] so depends only on a and not the particular Euclidean Jordan algebra in which it is calculated.
The compact set S is the set of extreme points of the closed unit ball ||x|| ≤ 1. Each u in S has norm one. Moreover, if u = eia and v = eib, then ||uv|| ≤ 1. Indeed, by the Cohn–Shirshov theorem the unital Jordan subalgebra of E generated by a and b is special. The inequality is easy to establish in non-exceptional simple Euclidean Jordan algebras, since each such Jordan algebra and its complexification can be realized as a subalgebra of some Hn(R) and its complexification Hn(C) ⊂ Mn(C). The spectral norm in Hn(C) is the usual operator norm. In that case, for unitary matrices U and V in Mn(C), clearly ||(UV + VU)|| ≤ 1. The inequality therefore follows in any special Euclidean Jordan algebra and hence in general.
On the other hand, by the Krein–Milman theorem, the closed unit ball is the (closed) convex span of S.[9] It follows that ||L(u)|| = 1, in the operator norm corresponding to either the inner product norm or spectral norm. Hence ||L(a)|| ≤ ||a|| for all a, so that the spectral norm satisfies
\displaystyle{\|ab\|\le\|a\| ⋅ \|b\|.}
It follows that EC is a Jordan C* algebra.
The complexification of a simple Euclidean Jordan algebra is a simple complex Jordan algebra which is also separable, i.e. its trace form is non-degenerate. Conversely, using the existence of a real form of the Lie algebra of the structure group, it can be shown that every complex separable simple Jordan algebra is the complexification of a simple Euclidean Jordan algebra.
To verify that the complexification of a simple Euclidean Jordan algebra E has no ideals, note that if F is an ideal in EC then so too is F⊥, the orthogonal complement for the trace norm. As in the real case, J = F⊥ ∩ F must equal (0). For the associativity property of the trace form shows that F⊥ is an ideal and that ab = 0 if a and b lie in J. Hence J is an ideal. But if z is in J, L(z) takes EC into J and J into (0). Hence Tr L(z) = 0. Since J is an ideal and the trace form degenerate, this forces z = 0. It follows that EC = F ⊕ F⊥. If P is the corresponding projection onto F, it commutes with the operators L(a) and F⊥ = (I − P)EC. is also an ideal and E = F ⊕ F⊥. Furthermore, if e = P(1), then P = L(e). In fact for a in E
\displaystyle{ea=ae=L(a)P(1)=P(L(a)1)=P(a),}
so that ea = a for a in F and 0 for a in F⊥. In particular e and 1 − e are orthogonal central idempotents with L(e) = P and L(1 − e) = I − P.
So simplicity follows from the fact that the center of EC is the complexification of the center of E.
According to the "elementary approach" to bounded symmetric space of Koecher,[10] Hermitian symmetric spaces of noncompact type can be realized in the complexification of a Euclidean Jordan algebra E as either the open unit ball for the spectral norm, a bounded domain, or as the open tube domain, where C is the positive open cone in E. In the simplest case where E = R, the complexification of E is just C, the bounded domain corresponds to the open unit disk and the tube domain to the upper half plane. Both these spaces have transitive groups of biholomorphisms given by Möbius transformations, corresponding to matrices in or . They both lie in the Riemann sphere, the standard one-point compactification of C. Moreover, the symmetry groups are all particular cases of Möbius transformations corresponding to matrices in . This complex Lie group and its maximal compact subgroup act transitively on the Riemann sphere. The groups are also algebraic. They have distinguished generating subgroups and have an explicit description in terms of generators and relations. Moreover, the Cayley transform gives an explicit Möbius transformation from the open disk onto the upper half plane. All these features generalize to arbitrary Euclidean Jordan algebras.[11] The compactification and complex Lie group are described in the next section and correspond to the dual Hermitian symmetric space of compact type. In this section only the symmetries of and between the bounded domain and tube domain are described.
Jordan frames provide one of the main Jordan algebraic techniques to describe the symmetry groups. Each Jordan frame gives rise to a product of copies of R and C. The symmetry groups of the corresponding open domains and the compactification—polydisks and polyspheres—can be deduced from the case of the unit disk, the upper halfplane and Riemann sphere. All these symmetries extend to the larger Jordan algebra and its compactification. The analysis can also be reduced to this case because all points in the complex algebra (or its compactification) lie in an image of the polydisk (or polysphere) under the unitary structure group.
Let be a Euclidean Jordan algebra with complexification .
The unit ball or disk D in is just the convex bounded open set of elements such the ||a|| < 1, i.e. the unit ball for the spectral norm.
The tube domain T in is the unbounded convex open set, where C is the open positive cone in .
The group SL(2,C) acts by Möbius transformations on the Riemann sphere C ∪, the one-point compactification of C. If g in SL(2,C) is given by the matrix
\displaystyle{g=\begin{pmatrix}\alpha&\beta\ \gamma&\delta\end{pmatrix},}
then
\displaystyle{g(z)=(\alphaz+\beta)(\gammaz+\delta)-1.}
Similarly the group SL(2,R) acts by Möbius transformations on the circle R ∪, the one-point compactification of R.
Let k = R or C. Then SL(2,k) is generated by the three subgroups of lower and upper unitriangular matrices, L and U', and the diagonal matrices D. It is also generated by the lower (or upper) unitriangular matrices, the diagonal matrices and the matrix
\displaystyle{J=\begin{pmatrix}0&1\ -1&0\end{pmatrix}.}
The matrix J corresponds to the Möbius transformation and can be written
\displaystyle{J=\begin{pmatrix}1&0\ -1&1\end{pmatrix}\begin{pmatrix}1&1\ 0&1\end{pmatrix} \begin{pmatrix}1&0\ -1&1\end{pmatrix}.}
The Möbius transformations fixing ∞ are just the upper triangular matrices B = UD = DU. If g does not fix ∞, it sends ∞ to a finite point a. But then g can be composed with an upper unitriangular matrix to send a to 0 and then with J to send 0 to infinity. This argument gives one of the simplest examples of the Bruhat decomposition:
\displaystyle{SL(2,k)=B\cupB ⋅ J ⋅ B,}
the double coset decomposition of . In fact the union is disjoint and can be written more precisely as
\displaystyle{SL(2,k)=B\cupB ⋅ J ⋅ U,}
where the product occurring in the second term is direct.
Now let
\displaystyle{T(\beta)=\begin{pmatrix}1&\beta\ 0&1\end{pmatrix}.}
Then
\displaystyle{\begin{pmatrix}\alpha&0\ 0&\alpha-1\end{pmatrix}=JT(\alpha-1)JT(\alpha)JT(\alpha-1).}
It follows is generated by the group of operators and J subject to the following relations:
The last relation follows from the definition of . The generator and relations above is fact gives a presentation of . Indeed, consider the free group Φ generated by J and with J of order 4 and its square central. This consists of all products for . There is a natural homomorphism of Φ onto . Its kernel contain the normal subgroup Δ generated by the relations above. So there is a natural homomorphism of Φ/Δ onto . To show that it is injective it suffices to show that the Bruhat decomposition also holds in . It is enough to prove the first version, since the more precise version follows from the commutation relations between J and. The set is invariant under inversion, contains operators and J, so it is enough to show it is invariant under multiplication. By construction it is invariant under multiplication by B. It is invariant under multiplication by J because of the defining equation for .
In particular the center of consists of the scalar matrices and it is the only non-trivial normal subgroup of, so that is simple. In fact if is a normal subgroup, then the Bruhat decomposition implies that is a maximal subgroup, so that either is contained in or. In the first case fixes one point and hence every point of, so lies in the center. In the second case, the commutator subgroup of is the whole group, since it is the group generated by lower and upper unitriangular matrices and the fourth relation shows that all such matrices are commutatorssince . Writing with in and in, it follows that . Since and generate the whole group, . But then . The right hand side here is Abelian while the left hand side is its own commutator subgroup. Hence this must be the trivial group and .
Given an element a in the complex Jordan algebra, the unital Jordan subalgebra is associative and commutative. Multiplication by a defines an operator on which has a spectrum, namely its set of complex eigenvalues. If is a complex polynomial, then is defined in . It is invertible in if and only if it is invertible in, which happen precisely when does not vanish on the spectrum of . This permits rational functions of to be defined whenever the function is defined on the spectrum of . If and are rational functions with and defined on, then is defined on and . This applies in particular to complex Möbius transformations which can be defined by. They leave invariant and, when defined, the group composition law holds. (In the next section complex Möbius transformations will be defined on the compactification of .)[12]
Given a primitive idempotent in with Peirce decomposition
\displaystyle{E=E1(e) ⊕ E1/2(e) ⊕ E0(e),A=A1(e) ⊕ A1/2(e) ⊕ A0(e).}
the action of by Möbius transformations on can be extended to an action on A so that the action leaves invariant the components and in particular acts trivially on . If is the projection onto, the action is given be the formula
\displaystyle{g(ze ⊕ x1/2 ⊕ x0)={\alphaz+\beta\over\gammaz+\delta} ⋅ e ⊕ (\gammaz+\delta)-1x1/2 ⊕ x0-(\gammaz+\delta)-1P0(x
| 2).} | |
| 1/2 |
For a Jordan frame of primitive idempotents, the actions of associated with different commute, thus giving an action of . The diagonal copy of gives again the action by Möbius transformations on .
See also: Cayley transform. The Möbius transformation defined by
\displaystyle{C(z)=i{1+z\over1-z}=-i+{2i\over1-z}}
is called the Cayley transform. Its inverse is given by
\displaystyle{P(w)={w-i\overw+i}=1-{2i\overw+i}.}
The inverse Cayley transform carries the real line onto the circle with the point 1 omitted. It carries the upper halfplane onto the unit disk and the lower halfplane onto the complement of the closed unit disk. In operator theory the mapping takes self-adjoint operators T onto unitary operators U not containing 1 in their spectrum. For matrices this follows because unitary and self-adjoint matrices can be diagonalized and their eigenvalues lie on the unit circle or real line. In this finite-dimensional setting the Cayley transform and its inverse establish a bijection between the matrices of operator norm less than one and operators with imaginary part a positive operator. This is the special case for of the Jordan algebraic result, explained below, which asserts that the Cayley transform and its inverse establish a bijection between the bounded domain and the tube domain .
In the case of matrices, the bijection follows from resolvant formulas. In fact if the imaginary part of is positive, then is invertible since
\displaystyle{\|(T+iI)x\|2=\|(T-iI)x\|2+4(Im(T)x,x).}
In particular, setting,
\displaystyle{\|y\|2=\|P(T)y\|2+4(Im(T)x,x).}
Equivalently
\displaystyle{I-P(T)*P(T)= 4(T*-iI)-1[ImT](T+iI)-1
is a positive operator, so that ||P(T)|| < 1. Conversely if ||U|| < 1 then is invertible and
\displaystyle{ImC(U)=(2i)-1[C(U)-C(U)*]= (1-U*)-1[I-U*U](I-U)-1.}
Since the Cayley transform and its inverse commute with the transpose, they also establish a bijection for symmetric matrices. This corresponds to the Jordan algebra of symmetric complex matrices, the complexification of .
In the above resolvant identities take the following form:[13]
\displaystyle{Q(1-u*)Q(C(u)+C(u*))Q(1-u)=-4B(u*,u)}
and equivalently
\displaystyle{4Q(Ima)=Q(a*-i)B(P(a)*,P(a))Q(a+i),}
where the Bergman operator is defined by with . The inverses here are well defined. In fact in one direction is invertible for ||u|| < 1: this follows either using the fact that the norm satisfies ||ab|| ≤ ||a|| ||b||; or using the resolvant identity and the invertibility of (see below). In the other direction if the imaginary part of is in then the imaginary part of is positive definite so that is invertible. This argument can be applied to, so it also invertible.
To establish the correspondence, it is enough to check it when is simple. In that case it follows from the connectivity of and and because:
The first criterion follows from the fact that the eigenvalues of are exactly if the eigenvalues of are . So the are either all positive or all negative. The second criterion follows from the fact that if with and u in, then has eigenvalues . So the are either all less than one or all greater than one.
The resolvant identity is a consequence of the following identity for and invertible
\displaystyle{Q(a)Q(a-1+b-1)Q(b)=Q(a+b).}
In fact in this case the relations for a quadratic Jordan algebra imply
\displaystyle{R(a,b)=2Q(a)Q(a-1,b)=2Q(a,b-1)Q(b)}
so that
\displaystyle{B(a,b)=Q(a)Q(a-1-b)=Q(b-1-a)Q(b).}
The equality of the last two terms implies the identity, replacing by .
Now set and . The resolvant identity is a special case of the more following more general identity:
\displaystyle{Q(1-x)Q(C(x)+C(y))Q(1-y)=-4B(x,y).}
In fact
\displaystyle{C(x)+C(y)=-2i(1-a-1-b-1),}
so the identity is equivalent to
\displaystyle{Q(a)Q(1-a-1-b-1)Q(b)=B(1-a,1-b).}
Using the identity above together with, the left hand side equals . The right hand side equals . These are equal because of the formula .
If is a biholomorphic mapping of onto itself just fixing 0 thenif, the mapping fixes 0 and has derivative there. It is therefore the identity map. So for any α. This implies g is a linear mapping. Since it maps onto itself it maps the closure onto itself. In particular it must map the Shilov boundary onto itself. This forces to be in the unitary structure group.
The orbit of 0 under AD is the set of all points with . The orbit of these points under the unitary structure group is the whole of . The Cartan decomposition follows because is the stabilizer of 0 in . In fact the only point fixed by (the identity component of) KD in D is 0. Uniqueness implies that the center of GD must fix 0. It follows that the center of GD lies in KD. The center of KD is isomorphic to the circle group: a rotation through θ corresponds to multiplication by eiθ on D so lies in . Since this group has trivial center, the center of GD is trivial.In fact any larger compact subgroup would intersect AD non-trivially and it has no non-trivial compact subgroups.Note that GD is a Lie group (see below), so that the above three statements hold with GD and KD replaced by their identity components, i.e. the subgroups generated by their one-parameter cubgroups. Uniqueness of the maximal compact subgroup up to conjugacy follows from a general argument or can be deduced for classical domains directly using Sylvester's law of inertia following .[14] For the example of Hermitian matrices over C, this reduces to proving that is up to conjugacy the unique maximal compact subgroup in . In fact if, then is the subgroup of preserving W. The restriction of the hermitian form given by the inner product on minus the inner product on .On the other hand, if is a compact subgroup of, there is a -invariant inner product on obtained by averaging any inner product with respect to Haar measure on . The Hermitian form corresponds to an orthogonal decomposition into two subspaces of dimension both invariant under with the form positive definite on one and negative definite on the other. By Sylvester's law of inertia, given two subspaces of dimension on which the Hermitian form is positive definite, one is carried onto the other by an element of . Hence there is an element of such that the positive definite subspace is given by . So leaves invariant and .
A similar argument, with quaternions replacing the complex numbers, shows uniqueness for the symplectic group, which corresponds to Hermitian matrices over R. This can also be seen more directly by using complex structures. A complex structure is an invertible operator J with J2 = −I preserving the symplectic form B and such that −B(Jx,y) is a real inner product. The symplectic group acts transitively on complex structures by conjugation. Moreover, the subgroup commuting with J is naturally identified with the unitary group for the corresponding complex inner product space. Uniqueness follows by showing that any compact subgroup K commutes with some complex structure J. In fact, averaging over Haar measure, there is a K-invariant inner product on the underlying space. The symplectic form yields an invertible skew-adjoint operator T commuting with K. The operator S = −T2 is positive, so has a unique positive square root, which commutes with K. So J = S−1/2T, the phase of T, has square −I and commutes with K.
There is a Cartan decomposition for GT corresponding to the action on the tube T = E + iC:
\displaystyle{GT=KTATKT.}
In fact the Cartan decomposition for follows from the decomposition for . Given in, there is an element in, the identity component of, such that with . Since ||z|| < 1, it follows that . Taking the Cayley transform of z, it follows that every in can be written, with the Cayley transform and in . Since with, the point is of the form with in . Hence .
There is an Iwasawa decomposition for GT corresponding to the action on the tube T = E + iC:
\displaystyle{GT=KTATNT.}
The group S = AN acts on E linearly and conjugation on N0 reproduces this action. Since the group S acts simply transitively on C, it follows that ANT=S⋅N0 acts simply transitively on T = E + iC. Let HT be the group of biholomorphisms of the tube T. The Cayley transform shows that is isomorphic to the group HD of biholomorphisms of the bounded domain D. Since ANT acts simply transitively on the tube T while KT fixes ic, they have trivial intersection.
Given g in HT, take s in ANT such that g−1(i)=s−1(i). then gs−1 fixes i and therefore lies in KT. Hence HT = KT ⋅A⋅NT. So the product is a group.
By a result of Henri Cartan, HD is a Lie group. Cartan's original proof is presented in . It can also be deduced from the fact the D is complete for the Bergman metric, for which the isometries form a Lie group; by Montel's theorem, the group of biholomorphisms is a closed subgroup.[15]
That HT is a Lie group can be seen directly in this case. In fact there is a finite-dimensional 3-graded Lie algebra
ak{g}T
ak{g}T
ak{g}T
ak{g}T
ak{g}T
ak{g}T
Euclidean Jordan algebras can be used to construct Hermitian symmetric spaces of tube type. The remaining Hermitian symmetric spaces are Siegel domains of the second kind. They can be constructed using Euclidean Jordan triple systems, a generalization of Euclidean Jordan algebras. In fact for a Euclidean Jordan algebra E let
\displaystyle{L(a,b)=2([L(a),L(b)]+L(ab)).}
Then L(a,b) gives a bilinear map into End E such that
\displaystyle{L(a,b)*=L(b,a)},L(a,b)c=L(c,b)a
and
\displaystyle{[L(a,b),L(c,d)]=L(L(a,b)c,d)-L(c,L(b,a)d).}
Any such bilinear system is called a Euclidean Jordan triple system. By definition the operators L(a,b) form a Lie subalgebra of End E.
The Kantor–Koecher–Tits construction gives a one-one correspondence between Jordan triple systems and 3-graded Lie algebras
\displaystyle{ak{g}=ak{g}-1 ⊕ ak{g}0 ⊕ ak{g}1,}
satisfying
\displaystyle{[ak{g}p,ak{g}q]\subseteqak{g}p+q
and equipped with an involutive automorphism σ reversing the grading. In this case
\displaystyle{L(a,b)=ad[a,\sigma(b)]}
defines a Jordan triple system on
ak{g}-1
ak{g}0
ak{h}
ak{g}\pm
\displaystyle{[(a1,T1,b1),(a2,T2,b2)]=(T1a2-T2a1,[T1,T2]+L(a1,b2)-L(a2,b1),T
| *b | |
| 1-T |
| *b | |
| 2)} |
and the involution by
\displaystyle{\sigma(a,T,b)=(b,-T*,a).}
The Killing form is given by
\displaystyle{B((a1,T1,b1),(a2,T2,b2))=(a1,b2)+(b1,a2)+\beta(T1,T2),}
where β(T1,T2) is the symmetric bilinear form defined by
\displaystyle{\beta(L(a,b),L(c,d))=(L(a,b)c,d)=(L(c,d)a,b).}
These formulas, originally derived for Jordan algebras, work equally well for Jordan triple systems.[16] The account in develops the theory of bounded symmetric domains starting from the standpoint of 3-graded Lie algebras. For a given finite-dimensional vector space E, Koecher considers finite-dimensional Lie algebras
ak{g}
ak{g}-1
ak{g}0
ak{g}\pm
ak{sl}2
The remaining cases are constructed uniformly by Koecher using involutions of simple Euclidean Jordan algebras. Let E be a simple Euclidean Jordan algebra and τ a Jordan algebra automorphism of E of period 2. Thus E = E+1 ⊕ E−1 has an eigenspace decomposition for τ with E+1 a Jordan subalgebra and E−1 a module. Moreover, a product of two elements in E−1 lies in E+1. For a, b, c in E−1, set
\displaystyle{L0(a,b)c=L(a,b)c}
and (a,b)= Tr L(ab). Then F = E−1 is a simple Euclidean Jordan triple system, obtained by restricting the triple system on E to F. Koecher exhibits explicit involutions of simple Euclidean Jordan algebras directly (see below). These Jordan triple systems correspond to irreducible Hermitian symmetric spaces given by Siegel domains of the second kind. In Cartan's listing, their compact duals are SU(p + q)/S(U(p) × U(q)) with p ≠ q (AIII), SO(2n)/U(n) with n odd (DIII) and E6/SO(10) × U(1) (EIII).
Examples
The classification of Euclidean Jordan triple systems has been achieved by generalizing the methods of Jordan, von Neumann and Wigner, but the proofs are more involved.[17] Prior differential geometric methods of, invoking a 3-graded Lie algebra, and of, lead to a more rapid classification.