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Compatible Peirce decompositions of Jordan triple systems - MSP

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64 KEVIN MCCRIMMON<br />

patibility reduces to<br />

1.13. COMPATIBILITY CRITERION FOR IDEMPOTENTS. TWO idempotents<br />

e, f in a <strong>Jordan</strong> algebra are compatible iff / = / 2 ® / 0 for<br />

orthogonal idempotents f tGJi(e).<br />

Pro<strong>of</strong>. The condition that / = α 2 + α L + a Q is idempotent is<br />

a 2 = at + E 2(e)a\<br />

(1.10') a1 — (α2 + αo) o<br />

α!<br />

α 0 = al + E 0(e)al<br />

and compatibility (1.11) becomes<br />

(1.110 αo 0<br />

^ + αχoα2 = 0 ,<br />

hence a λ — 0 and α 2 = α^ α 0 = αξ are orthogonal idempotents. Conversely,<br />

if /= / 2 + /o then e, / are compatible by (1.8iv). Π<br />

Note that the strong compatibility condition that the operators<br />

P(e), L(e, e) commute with P(f), L(f f) (not merely P(e) 2<br />

and P(/) 2<br />

)<br />

is not an intrinsic condition: it depends on how e, f are imbedded<br />

in J. For example, e = 1[12] and / = 1[13] are collinear and strongly<br />

compatible in £>[12]+D[13] = MU2(D), but not in HID) since P(e)P(f)<br />

1[33] - P(β)l[ll] = 1[22] Φ 0 = P(/)P(e)l[33].<br />

The most important examples <strong>of</strong> compatible tripotents are either<br />

orthogonal e _L / (each lies in the 0-space <strong>of</strong> the other) or collinear<br />

eTf (each lies in the 1-space <strong>of</strong> the other). In the remainder <strong>of</strong><br />

this section we investigate what collinearity amounts to in basic<br />

examples <strong>of</strong> <strong>triple</strong> <strong>systems</strong>. Recall that tripotents e, f are collinear<br />

if P(e)f - P(/)e - 0, L(e, e)f = /, L(f f f)e = e.<br />

Let us note that in a <strong>Jordan</strong> algebra we cannot have collinear<br />

idempotents; collinearity is strictly for tripotents.<br />

PROPOSITION 1.14. Two nonzero idempotents in a <strong>Jordan</strong> algebra<br />

can never be collinear.<br />

Pro<strong>of</strong>. If eeJjif) and feJ^e) are idempotents then f—{eef)~<br />

e 2 <strong>of</strong> = e <strong>of</strong>=e<strong>of</strong>= {eff} = e, so /= P(/)/= P(f)e - 0 and dually<br />

e = 0. (Alternately, if feJ,(e) then / 2 6 J 2(e) + J 0(e), so the only<br />

idempotent in J^e) is / = 0. Or yet again, the result follows directly<br />

from (1.13).) D

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