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Compatible Peirce decompositions of Jordan triple systems - MSP

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COMPATIBLE PEIRCE DECOMPOSITIONS OF JORDAN TRIPLE SYSTEMS 67<br />

forms a family <strong>of</strong> hermitian matrix units and thus yields an imbedding<br />

H Z(Φ) —• / sending l[ii] -> e if l[ij] -> ι%. •<br />

Collinearity in JT(A, *)<br />

A more general method for obtaining <strong>Jordan</strong> <strong>triple</strong>s T from<br />

<strong>Jordan</strong> algebras J is through P(x)y — U(x)y* for some involution *<br />

<strong>of</strong> J. However, there seems to be no relation between tripotents<br />

x e JT(J, *) and idempotents in J (in general there don't seem to be<br />

idempotents in J). In the special case where / = A +<br />

, so P(x)y =<br />

xy*x, an element x is tripotent iff x — a + δ for aeeAe, beeA(l — e)<br />

satisfying αα* + 66* = e for a symmetric idempotent β (namely e =<br />

a%c*, a = xe, 6 = a;(l — e)). Collinearity becomes complicated,<br />

1.20. COLLINEARITY THEOREM FOR JT(A, *). Two nonzero tripotents<br />

x, y in JT(A, *) are collinear iff £/&erβ are £wo families e n,<br />

€22, β 33 a^cί / n, / 22, / 33 o/ symmetric orthogonal idempotents and elements<br />

x ijf y i3' in e uAf 5j such that<br />

x = x 12 + x 21, y = y 13 + y 31<br />

Pro<strong>of</strong>. a->a' = (\ Q) imbeds JΓ(A, *) in JΓ(B) for B=Λf 2(il),<br />

so from (1.15) ^' - eί 2 + e 21, y' = eί s + ώ for ej,.= ^ t °Q j<br />

\i, j = 1, 2)<br />

^4 = (°/Q) (i, fc = 1, 3), e'u = ^Q* ?) we get the result. Π<br />

2* <strong>Compatible</strong> <strong>Peirce</strong> decomposition* A finite family gf —<br />

{βi, , en } <strong>of</strong> tripotents is compatible if every pair eif e3- is compatible.<br />

Now any time we have a finite number <strong>of</strong> commuting <strong>decompositions</strong><br />

I — Eziβi) + E^βi) + E0 (ei) relative to eu them together to get a simultaneous decomposition<br />

, en we can put<br />

<strong>of</strong> the identity operator for<br />

Σ<br />

(i I , .i Λ )e{2,l,0} Λ<br />

By commutativity these JSΓS are supplementary projection operators,<br />

and hence yield a compatible <strong>Peirce</strong> decomposition.<br />

J — © ^ (ϊi, ,ί Λ )<br />

(2.1) « 1 . .i,)βu, 1 .θ!.

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