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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98 KEVIN MCGRIMMON<br />
S and S* preserve <strong>Peirce</strong> spaces relative to e> S(J k (e)) + S*(J k (e))(Z<br />
M k (e) for k = 2, 1, 0, iff S and S* preserve e in the sense that S(e),<br />
S*(e) e M 2 (e). Always S'= S - {L(m lf e) + L(e, m,)} has S\e), S'*(β) 6<br />
M 2 (e) so we can modify S by an inner multiplication to obtain S'<br />
preserving <strong>Peirce</strong> spaces. If S = D is a derivation then L(m u e) +<br />
L(e, mj = D(m lf e) is a standard inner derivation.<br />
Pro<strong>of</strong>. If S(e) = m = Σ w,, S*(e) = m* = Σ ^f for m*, m? 6<br />
Λfi(β) then by (7.1) S(P(e)e) + P(e)S*(e) = {S(e)ee} implies (m 2 + m^<br />
m 0) + m 2* = 2m 2 + m 2, hence m 0 = 0 and m$ = m 2. Dually m* = 0<br />
and m 2 = m 2. This establishes (i).<br />
For XiβJiie) the linearized varsion <strong>of</strong> (7.1) yields S({eeXi}) +<br />
icJ = {a?iβjS(β)} + {eeS(Xi)} 9 hence ΐS(^) + {emtXi} + {emtxt} =<br />
+ {m^α J + L(e, e)S(Xt). But L(e, m?) = L(mF, e)=L(m2 f β) by<br />
(i) and (1.4) so<br />
{L{e, e) ~ U}S(Xi) = {emfίcj — {m^Xi} .<br />
For ΐ = 1 taking components in M2, Mo yields (iv). For i = 0 we<br />
get the expression (iii) for EβiXo), where S(xo)eMo + Mλ since by<br />
(7.1) P(e)S(x0) = -S*(P(e)a? 0) + {S*(βKe} = 0. For ΐ = 2 we get the<br />
expression (ii) for EβiXz), where S(x2)eM2+M1 since by (7.1) S(x2) =<br />
S(P(e)x2) = -P(e)S*(xt) + {S(e)x2e} e P(e)M + {eJM}.<br />
If J is locally unital then S{J)^S(^ J2{e,)) c.^ Afβ(ef)+Λfι(e