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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

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