A Cayley-Dickson process for a class of structurable algebras
A Cayley-Dickson process for a class of structurable algebras
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DOI:
10.1090/s0002-9947-1984-0735416-2
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发表时间:
1984
影响因子:
1.3
通讯作者:
B. Allison;J. Faulkner
中科院分区:
文献类型:
--
作者:
B. Allison;J. Faulkner
In this paper, we study the class of all simple structurable algebras with the property that the space of skew-hermitian elements has dimension 1. These algebras with involution have arisen in the study of Lie algebra constructions. The reduced algebras are isotopic to 2 X 2 matrix algebras. We study a Cayley-Dickson process for rationally constructing some algebras in the class including division algebras and nonreduced nondivision algebras. An important special case of the process endows the direct sum of two copies of a 28-dimensional degree 4 central simple Jordan algebra © with the structure of an algebra with involution. In preparatory work, we obtain a procedure for giving the space ©0 of trace zero elements of any such Jordan algebra © the structure of a 27-dimensional exceptional Jordan algebra. The 56-dimensional irreducible module 911 for the split simple Lie algebra of type E1 over a field I possesses the structure of an algebra with involution that can be used in the construction of the split simple Lie algebras of type £7 and £8 [2,5 and 11]. In order to study nonsplit Lie algebras of these types, it is of interest to have a rational (in the sense that base field extension is not involved) construction of f-forms of 91Lj, where I denotes the algebraic closure of f and a f-form of 911 ̂ is an algebra with involution (&,') over f such that (&,~)'f = 9Hf. The underlying vector space for 911 is the vector space of all 2 X 2 matrices with scalar diagonal entries and nondiagonal entries chosen from the 27-dimensional split exceptional central simple Jordan algebra. The multiplication on 911 is strikingly similar to the multiplication on the split octonion algebra 0 over f as obtained from the Zorn construction [9, p. 142]. Thus, it is natural to ask whether there is a Cayley-Dickson process for constructing f-forms 911 ̂ that is analogous to the classical Cayley-Dickson process for constructing f-forms of 0j [15, p. 45]. We will see that a f-form of 911 f can be constructed by endowing the direct sum of two copies of a 28-dimensional degree 4 central simple Jordan algebra with the structure of an algebra with involution (see Example 6.12). This construction is a special case of the Cayley-Dickson process that is the main subject of this paper. In [1], a class of algebras with involution called structurable algebras was studied. The matrix algebra 911 referred to in the previous paragraph is an example of a Received by the editors April 1, 1983. 1980 Mathematics Subject Classification. Primary 17A30; Secondary 17B60, 17C20. 1 Research supported in part by an NSERC Grant. 2 Research supported in part by an NSF Grant. ©1984 American Mathematical Society 0025-5726/84 $1.00 + $.25 per page 185 License or copyright restrictions may apply to redistribution; see https://www.ams.org/journal-terms-of-use 186 B.N. ALLISON AND J. R. FAULKNER simple structurable algebra (&,') such that space §((£,")= (x E tP|x = -x} has dimension 1. In §§1-4, we investigate the class of all simple structurable algebras (&,') such that §((J,") has dimension 1. Any such algebra (&,~) possesses a quartic form v that occurs naturally as the denominator in the inversion operation. This quartic form gives (&,') the structure of a Freudenthal triple system and thereby allows us to make use of earlier work of Ferrar on such systems. The Cayley-Dickson process studied in this paper has as its starting point a Jordan algebra possessing a Jordan norm of degree 4. These norms are studied in §5. An example of a Jordan norm of degree 4 is the generic norm on a degree 4 separable Jordan algebra. We obtain as a consequence of our work in §5 the fact that the space of trace 0 elements in a degree 4 separable Jordan algebra has the structure of a degree 3 separable Jordan algebra. In particular, starting with a 28-dimensional central simple degree 4 (special) Jordan algebra, a 27-dimensional exceptional central simple Jordan algebra is obtained. In §6 we describe the Cayley-Dickson process that produces simple structurable algebras (&, ~) such that dimt S(6E, ~) = 1. In §7, we show that for certain choices of the parameters the process produces division algebras. We also discuss in §7 the use of such algebras in the construction of exceptional central simple Lie algebras over a field of characteristic zero. Finally, in §8, we give necessary and sufficient conditions for the process to give reduced algebras. Before proceeding, we fix some conventions and notation. Throughout the paper, we assume that I is field of characteristic =£2 or 3. All vector spaces and algebras over I are assumed to be finite dimensional over I. Algebras are not necessarily assumed to be associative and (except for Lie algebras) all algebras are assumed to possess a multiplicative identity denoted by 1. If & is an algebra and x, y, z E 6B, we write [x, y, z] = (xy)z — x(yz). An algebra with involution (6?,") is an algebra t? together with an anti-isomorphism x -» x of period two. If (&, ') is an algebra with involution, we denote the spaces of hermitian and skew-hermitian elements by %(&,-)= {xE&\x = x} and §(#,") = {x £ &\x = -x], in which case & = %(&, ~) © S(ffi,"). Finally, suppose Tis a vector space over t and m is a nonnegative integer dbFis linear. The authors wish to express their gratitude to the referee for several helpful suggestions. License or copyright restrictions may apply to redistribution; see https://www.ams.org/journal-terms-of-use A CAYLEY-DICKSON PROCESS 187 1. Structurable algebras. We collect in this section the facts about structurable algebras that will be used in later sections. An algebra with involution ((£,") over f is called a structurable algebra if for x, y, z, w E 6£, where V E Endt(6£) is defined by Vxyz = {x, y, z) = (xy)z + (zy)x (zx)y. We assume for the rest of the section that (6B,"") is a structurable algebra over t. We write § = S(fcV) and % = %(&,'). Define ^: & X 6t -» § by ^s>-,(jc, j) = x/ — jx. If no ambiguity exists, we write \p — *Pt&,-y Note that \[/(s, 1) = 2s for s E § and so ^ is a surjection. For x, z E &, define L/._,, Lx, Rx, and (/ E Endt(6E) by Ux :y — Vx z, Lxy = xy, Rxy = yx, and Ux — Uxx. Then we have the following identities for x, y E &, s E S (see [1, §1], [2, Lemma 2], and [3, §11]): (1.2) [s,x, y] = -[x,s, y] = [x, y, s], v'-V "jt,^ ~~ "y.sx A^x,>>).*' (1.5) s^(x, j)s =-i//(sx,5y), and 0-6) LJJXtyL, = -UJXt,y. Also 0 = [KIf,, Fx>>,] = K{JWt}>J1 F^^, (by (1.1)) and so (L?) ^=^ for x, y E 6E. Thus, if x E 6E and s E S, ^{x,iJT,x},ix 'x,{jx,^,ijr) — * x,s{x,sx,x) \"J V'1^// ^{x,jx,x},5x + ^4,(x,{X,sx,x})Ls (by (1-4)).