Triple system

In algebra, a triple system (or ternar) is a vector space V over a field F together with a F-trilinear map

${\displaystyle (\cdot ,\cdot ,\cdot )\colon V\times V\times V\to V.}$

The most important examples are Lie triple systems and Jordan triple systems. They were introduced by Nathan Jacobson in 1949 to study subspaces of associative algebras closed under triple commutators [[u, v], w] and triple anticommutators {u, {v, w}}. In particular, any Lie algebra defines a Lie triple system and any Jordan algebra defines a Jordan triple system. They are important in the theories of symmetric spaces, particularly Hermitian symmetric spaces and their generalizations (symmetric R-spaces and their noncompact duals).

A triple system is said to be a Lie triple system if the trilinear map, denoted ${\displaystyle [\cdot ,\cdot ,\cdot ]}$, satisfies the following identities:

${\displaystyle [u,v,w]=-[v,u,w]}$

${\displaystyle [u,v,w]+[w,u,v]+[v,w,u]=0}$

${\displaystyle [u,v,[w,x,y]]=[[u,v,w],x,y]+[w,[u,v,x],y]+[w,x,[u,v,y]].}$

The first two identities abstract the skew symmetry and Jacobi identity for the triple commutator, while the third identity means that the linear map L_u,v: V → V, defined by L_u,v(w) = [u, v, w], is a derivation of the triple product. The identity also shows that the space k = span {L_u,v : u, v ∈ V} is closed under commutator bracket, hence a Lie algebra.

Writing m in place of V, it follows that

${\displaystyle {\mathfrak {g}}:=k\oplus {\mathfrak {m}}}$

can be made into a ${\displaystyle \mathbb {Z} _{2}}$-graded Lie algebra, the standard embedding of m, with bracket

${\displaystyle [(L,u),(M,v)]=([L,M]+L_{u,v},L(v)-M(u)).}$

The decomposition of g is clearly a symmetric decomposition for this Lie bracket, and hence if G is a connected Lie group with Lie algebra g and K is a subgroup with Lie algebra k, then G/K is a symmetric space.

Conversely, given a Lie algebra g with such a symmetric decomposition (i.e., it is the Lie algebra of a symmetric space), the triple bracket [[u, v], w] makes m into a Lie triple system.

A triple system is said to be a Jordan triple system if the trilinear map, denoted {.,.,.}, satisfies the following identities:

${\displaystyle \{u,v,w\}=\{u,w,v\}}$

${\displaystyle \{u,v,\{w,x,y\}\}=\{w,x,\{u,v,y\}\}+\{w,\{u,v,x\},y\}-\{\{v,u,w\},x,y\}.}$

The first identity abstracts the symmetry of the triple anticommutator, while the second identity means that if L_u,v:V→V is defined by L_u,v(y) = {u, v, y} then

${\displaystyle [L_{u,v},L_{w,x}]:=L_{u,v}\circ L_{w,x}-L_{w,x}\circ L_{u,v}=L_{w,\{u,v,x\}}-L_{\{v,u,w\},x}}$

so that the space of linear maps span {L_u,v:u,v ∈ V} is closed under commutator bracket, and hence is a Lie algebra g₀.

Any Jordan triple system is a Lie triple system with respect to the product

${\displaystyle [u,v,w]=\{u,v,w\}-\{v,u,w\}.}$

A Jordan triple system is said to be positive definite (resp. nondegenerate) if the bilinear form on V defined by the trace of L_u,v is positive definite (resp. nondegenerate). In either case, there is an identification of V with its dual space, and a corresponding involution on g₀. They induce an involution of

${\displaystyle V\oplus {\mathfrak {g}}_{0}\oplus V^{*}}$

which in the positive definite case is a Cartan involution. The corresponding symmetric space is a symmetric R-space. It has a noncompact dual given by replacing the Cartan involution by its composite with the involution equal to +1 on g₀ and −1 on V and V^*. A special case of this construction arises when g₀ preserves a complex structure on V. In this case we obtain dual Hermitian symmetric spaces of compact and noncompact type (the latter being bounded symmetric domains).

A Jordan pair is a generalization of a Jordan triple system involving two vector spaces V₊ and V₋. The trilinear map is then replaced by a pair of trilinear maps

${\displaystyle \{\cdot ,\cdot ,\cdot \}_{+}\colon V_{-}\times S^{2}V_{+}\to V_{+}}$

${\displaystyle \{\cdot ,\cdot ,\cdot \}_{-}\colon V_{+}\times S^{2}V_{-}\to V_{-}}$

which are often viewed as quadratic maps V₊ → Hom(V₋, V₊) and V₋ → Hom(V₊, V₋). The other Jordan axiom (apart from symmetry) is likewise replaced by two axioms, one being

${\displaystyle \{u,v,\{w,x,y\}_{+}\}_{+}=\{w,x,\{u,v,y\}_{+}\}_{+}+\{w,\{u,v,x\}_{+},y\}_{+}-\{\{v,u,w\}_{-},x,y\}_{+}}$

and the other being the analogue with + and − subscripts exchanged.

As in the case of Jordan triple systems, one can define, for u in V₋ and v in V₊, a linear map

${\displaystyle L_{u,v}^{+}:V_{+}\to V_{+}\quad {\text{by}}\quad L_{u,v}^{+}(y)=\{u,v,y\}_{+}}$

and similarly L⁻. The Jordan axioms (apart from symmetry) may then be written

${\displaystyle [L_{u,v}^{\pm },L_{w,x}^{\pm }]=L_{w,\{u,v,x\}_{\pm }}^{\pm }-L_{\{v,u,w\}_{\mp },x}^{\pm }}$

which imply that the images of L⁺ and L⁻ are closed under commutator brackets in End(V₊) and End(V₋). Together they determine a linear map

${\displaystyle V_{+}\otimes V_{-}\to {\mathfrak {gl}}(V_{+})\oplus {\mathfrak {gl}}(V_{-})}$

whose image is a Lie subalgebra ${\displaystyle {\mathfrak {g}}_{0}}$, and the Jordan identities become Jacobi identities for a graded Lie bracket on

${\displaystyle V_{+}\oplus {\mathfrak {g}}_{0}\oplus V_{-},}$

so that conversely, if

${\displaystyle {\mathfrak {g}}={\mathfrak {g}}_{+1}\oplus {\mathfrak {g}}_{0}\oplus {\mathfrak {g}}_{-1}}$

is a graded Lie algebra, then the pair ${\displaystyle ({\mathfrak {g}}_{+1},{\mathfrak {g}}_{-1})}$ is a Jordan pair, with brackets

${\displaystyle \{X_{\mp },Y_{\pm },Z_{\pm }\}_{\pm }:=[[X_{\mp },Y_{\pm }],Z_{\pm }].}$

Jordan triple systems are Jordan pairs with V₊ = V₋ and equal trilinear maps. Another important case occurs when V₊ and V₋ are dual to one another, with dual trilinear maps determined by an element of

${\displaystyle \mathrm {End} (S^{2}V_{+})\cong S^{2}V_{+}^{*}\otimes S^{2}V_{-}^{*}\cong \mathrm {End} (S^{2}V_{-}).}$

These arise in particular when ${\displaystyle {\mathfrak {g}}}$ above is semisimple, when the Killing form provides a duality between ${\displaystyle {\mathfrak {g}}_{+1}}$ and ${\displaystyle {\mathfrak {g}}_{-1}}$.

• Associator
• Quadratic Jordan algebra

• Bertram, Wolfgang (2000), The geometry of Jordan and Lie structures, Lecture Notes in Mathematics, vol. 1754, Springer, ISBN 978-3-540-41426-1
• Helgason, Sigurdur (2001) [1978], Differential geometry, Lie groups, and symmetric spaces, Graduate Studies in Mathematics, vol. 34, American Mathematical Society, ISBN 978-0-8218-2848-9

• Jacobson, Nathan (1949), "Lie and Jordan triple systems", American Journal of Mathematics, 71 (1): 149–170, doi:10.2307/2372102, JSTOR 2372102
• Kamiya, Noriaki (2001) [1994], "Lie triple system", Encyclopedia of Mathematics, EMS Press.
• Kamiya, Noriaki (2001) [1994], "Jordan triple system", Encyclopedia of Mathematics, EMS Press.
• Koecher, M. (1969), An elementary approach to bounded symmetric domains, Lecture Notes, Rice University
• Loos, Ottmar (1969), General Theory, Symmetric spaces, vol. 1, W. A. Benjamin, OCLC 681278693
• Loos, Ottmar (1969), Compact Spaces and Classification, Symmetric spaces, vol. 2, W. A. Benjamin
• Loos, Ottmar (1971), "Jordan triple systems, R-spaces, and bounded symmetric domains", Bulletin of the American Mathematical Society, 77 (4): 558–561, doi:10.1090/s0002-9904-1971-12753-2
• Loos, Ottmar (2006) [1975], Jordan pairs, Lecture Notes in Mathematics, vol. 460, Springer, ISBN 978-3-540-37499-2
• Loos, Ottmar (1977), Bounded symmetric domains and Jordan pairs (PDF), Mathematical lectures, University of California, Irvine, archived from the original (PDF) on 2016-03-03
• Meyberg, K. (1972), Lectures on algebras and triple systems (PDF), University of Virginia
• Rosenfeld, Boris (1997), Geometry of Lie groups, Mathematics and its Applications, vol. 393, Kluwer, p. 92, ISBN 978-0792343905, Zbl 0867.53002
• Tevelev, E. (2002), "Moore-Penrose inverse, parabolic subgroups, and Jordan pairs", Journal of Lie Theory, 12: 461–481, arXiv:math/0101107, Bibcode:2001math......1107T