Compatible Peirce decompositions of Jordan triple systems - MSP
Compatible Peirce decompositions of Jordan triple systems - MSP
Compatible Peirce decompositions of Jordan triple systems - MSP
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COMPATIBLE PEIRCE DECOMPOSITIONS OF JORDAN TRIPLE SYSTEMS 65<br />
Collinearity in JT{A)<br />
From any associative algebra A we can form a <strong>Jordan</strong> <strong>triple</strong><br />
system JT(A) on the linear space A by<br />
P(x)y — xyx .<br />
Here an element x is tripotent iSxxx = x, i.e., # 8 = x. In this ease<br />
e = a; 2<br />
is an ordinary associative idempotent, and e# = xe = #, Thus<br />
x lies in the unital <strong>Peirce</strong> subalgebra eAe and is a "square root <strong>of</strong><br />
unity" therein. Examples <strong>of</strong> collinear tripotents are the matrix<br />
units x = E12, y — E1Z or & = i£ 12 + i? 21, V = Eu + E91. The latter<br />
example is quite general, since we have<br />
1.15. COLLINEARITY THEOREM FOR JT(A). TWO nonzero tripotents<br />
x, y in JT(A) are collinear iff there is a subalgebra B = M Z(Φ) <strong>of</strong><br />
A with x = E ί2 + E 21, y ^ E 1Z + E Z1.<br />
Pro<strong>of</strong>. Tripotence means x* = x, y z<br />
= y and collinearity means<br />
xyx = 2/#2/ = 0> x*V + 2/^ 2<br />
= l/> y 2<br />
% + ί»2/ 2<br />
= «• Then x 2<br />
y 2<br />
—(y—yx 2<br />
)y—<br />
y(y — x 2<br />
y) — y z<br />
% 2<br />
, so a direct calculation shows<br />
e n = x 2 2/ 2 = 2/V β 22 = αjί/ 2 a; e S5 — yx 2 y<br />
form a complete family <strong>of</strong> matrix units, hence yield an isomorphism<br />
<strong>of</strong> M Z(Φ) into A by E iά -> e