J-structure
In mathematics, a J-structure is an algebraic structure over a field related to a Jordan algebra. The concept was introduced by Springer (1973) to develop a theory of Jordan algebras using linear algebraic groups and axioms taking the Jordan inversion as basic operation and Hua's identity as a basic relation. There is a classification of simple structures deriving from the classification of semisimple algebraic groups. Over fields of characteristic not equal to 2, the theory of J-structures is essentially the same as that of Jordan algebras.
Definition
Let V be a finite-dimensional vector space over a field K and j a rational map from V to itself, expressible in the form n/N with n a polynomial map from V to itself and N a polynomial in K[V]. Let H be the subset of GL(V) × GL(V) containing the pairs (g,h) such that g∘j = j∘h: it is a closed subgroup of the product and the projection onto the first factor, the set of g which occur, is the structure group of j, denoted G'(j).
A J-structure is a triple (V,j,e) where V is a vector space over K, j is a birational map from V to itself and e is a non-zero element of V satisfying the following conditions.[1]
- j is a homogeneous birational involution of degree −1
- j is regular at e and j(e) = e
- if j is regular at x, e + x and e + j(x) then
- the orbit G e of e under the structure group G = G(j) is a Zariski open subset of V.
The norm associated to a J-structure (V,j,e) is the numerator N of j, normalised so that N(e) = 1. The degree of the J-structure is the degree of N as a homogeneous polynomial map.[2]
The quadratic map of the structure is a map P from V to End(V) defined in terms of the differential dj at an invertible x.[3] We put
The quadratic map turns out to be a quadratic polynomial map on V.
The subgroup of the structure group G generated by the invertible quadratic maps is the inner structure group of the J-structure. It is a closed connected normal subgroup.[4]
J-structures from quadratic forms
Let K have characteristic not equal to 2. Let Q be a quadratic form on the vector space V over K with associated bilinear form Q(x,y) = Q(x+y) − Q(x) − Q(y) and distinguished element e such that Q(e,.) is not trivial. We define a reflection map x* by
and an inversion map j by
Then (V,j,e) is a J-structure.
Example
Let Q be the usual sum of squares quadratic function on Kr for fixed integer r, equipped with the standard basis e1,...,er. Then (Kr, Q, er) is a J-structure of degree 2. It is denoted O2.[5]
Link with Jordan algebras
In characteristic not equal to 2, which we assume in this section, the theory of J-structures is essentially the same as that of Jordan algebras.
Let A be a finite-dimensional commutative non-associative algebra over K with identity e. Let L(x) denote multiplication on the left by x. There is a unique birational map i on A such that i(x).x = e if i is regular on x: it is homogeneous of degree −1 and an involution with i(e) = e. It may be defined by i(x) = L(x)−1.e. We call i the inversion on A.[6]
A Jordan algebra is defined by the identity[7][8]
An alternative characterisation is that for all invertible x we have
If A is a Jordan algebra, then (A,i,e) is a J-structure. If (V,j,e) is a J-structure, then there exists a unique Jordan algebra structure on V with identity e with inversion j.
Link with quadratic Jordan algebras
In general characteristic, which we assume in this section, J-structures are related to quadratic Jordan algebras. We take a quadratic Jordan algebra to be a finite dimensional vector space V with a quadratic map Q from V to End(V) and a distinguished element e. We let Q also denote the bilinear map Q(x,y) = Q(x+y) − Q(x) − Q(y). The properties of a quadratic Jordan algebra will be[9][10]
- Q(e) = idV, Q(x,e)y = Q(x,y)e
- Q(Q(x)y) = Q(x)Q(y)Q(x)
- Q(x)Q(y,z)x = Q(Q(x)y,x)z
We call Q(x)e the square of x. If the squaring is dominant (has Zariski dense image) then the algebra is termed separable.[11]
There is a unique birational involution i such that Q(x)i x = x if Q is regular at x. As before, i is the inversion, definable by i(x) = Q(x)−1 x.
If (V,j,e) is a J-structure, with quadratic map Q then (V,Q,e) is a quadratic Jordan algebra. In the opposite direction, if (V,Q,e) is a separable quadratic Jordan algebra with inversion i, then (V,i,e) is a J-structure.[12]
H-structure
McCrimmon proposed a notion of H-structure by dropping the density axiom and strengthening the third (a form of Hua's identity) to hold in all isotopes. The resulting structure is categorically equivalent to a quadratic Jordan algebra.[13][14]
Peirce decomposition
A J-structure has a Peirce decomposition into subspaces determined by idempotent elements.[15] Let a be an idempotent of the J-structure (V,j,e), that is, a2 = a. Let Q be the quadratic map. Define
This is invertible for non-zero t,u in K and so φ defines a morphism from the algebraic torus GL1 × GL1 to the inner structure group G1. There are subspaces
and these form a direct sum decomposition of V. This is the Peirce decomposition for the idempotent a.[16]
Generalisations
If we drop the condition on the distinguished element e, we obtain "J-structures without identity".[17] These are related to isotopes of Jordan algebras.[18]
References
- ↑ Springer (1973) p.10
- ↑ Springer (1973) p.11
- ↑ Springer (1973) p.16
- ↑ Springer (1973) p.18
- ↑ Springer (1973) p.33
- ↑ Springer (1973) p.66
- ↑ Schafer (1995) p.91
- ↑ Okubo (2005) p.13
- ↑ Springer (1973) p.72
- ↑ McCrimmon (2004) p.83
- ↑ Springer (1973) p.74
- ↑ Springer (1973) p.76
- ↑ McCrimmon (1977)
- ↑ McCrimmon (1978)
- ↑ Springer (1973) p.90
- ↑ Springer (1973) p.92
- ↑ Springer (1973) p.21
- ↑ Springer (1973) p.22
- McCrimmon, Kevin (1977). "Axioms for inversion in Jordan algebras". J. Algebra 47: 201–222. doi:10.1016/0021-8693(77)90221-6. Zbl 0421.17013.
- McCrimmon, Kevin (1978). "Jordan algebras and their applications". Bull. Am. Math. Soc. 84: 612–627. doi:10.1090/S0002-9904-1978-14503-0. MR 0466235. Zbl 0421.17010.
- McCrimmon, Kevin (2004). A taste of Jordan algebras. Universitext. Berlin, New York: Springer-Verlag. doi:10.1007/b97489. ISBN 978-0-387-95447-9. MR 2014924. Zbl 1044.17001.
- Okubo, Susumu (2005) [1995]. Introduction to Octonion and Other Non-Associative Algebras in Physics. Montroll Memorial Lecture Series in Mathematical Physics 2. Cambridge University Press. doi:10.1017/CBO9780511524479. ISBN 0-521-01792-0. Zbl 0841.17001.
- Schafer, Richard D. (1995) [1966]. An Introduction to Nonassociative Algebras. Dover. ISBN 0-486-68813-5. Zbl 0145.25601.
- Springer, T.A. (1973). Jordan algebras and algebraic groups. Ergebnisse der Mathematik und ihrer Grenzgebiete 75. Berlin-Heidelberg-New York: Springer-Verlag. ISBN 3-540-06104-5. Zbl 0259.17003.