Bourbaki

Proposition 1

Tag 066F, permanent. Cite it as [Bourbaki, Tag 066F].

Algebra, chapter III, § 10. Derivations

Let d1,d2d_1, d_2 be two ε\varepsilon-derivations of (A,A′,A′′)(A, A', A'') of respective degrees δ1,δ2\delta_1, \delta_2. Then the ε\varepsilon-bracket

[d1,d2]ε=d1∘d2−εδ1,δ2d2∘d1 [d_1, d_2]_\varepsilon = d_1 \circ d_2 - \varepsilon_{\delta_1, \delta_2} d_2 \circ d_1
is an ε\varepsilon-derivation of degree δ1+δ2\delta_1 + \delta_2. Moreover, if dd is an ε\varepsilon-derivation of (A,A′,A′′)(A, A', A'') of degree δ\delta and if εδ,δ=−1\varepsilon_{\delta, \delta} = -1, then d2=d∘dd^2 = d \circ d is a derivation.

Suppose x∈Ax \in A is homogeneous of degree ξ\xi; for all y∈A′y \in A',

d1(d2(xy))=((d1d2)(x))y+εδ1,δ2+ξ(d2x)(d1y)+εδ2,ξ(d1x)(d2y)+εδ1+δ2,ξx((d1d2)(y)) d_1(d_2(xy)) = ((d_1 d_2)(x))y + \varepsilon_{\delta_1, \delta_2 + \xi}(d_2 x)(d_1 y) + \varepsilon_{\delta_2, \xi}(d_1 x)(d_2 y) + \varepsilon_{\delta_1 + \delta_2, \xi} x((d_1 d_2)(y))
taking account of formulae (1) of no. 1. Exchanging the roles of d1d_1 and d2d_2, we obtain, after simplifications again using (1) (no. 1),
(d1d2)(xy)−εδ1,δ2(d2d1)(xy)=((d1d2)(x))y−εδ1,δ2((d2d1)(x))y+εδ1+δ2,ξx((d1d2)(y))−εδ1,δ2εδ1+δ2,ξx((d2d1)(y)) (d_1 d_2)(xy) - \varepsilon_{\delta_1, \delta_2}(d_2 d_1)(xy) = ((d_1 d_2)(x))y - \varepsilon_{\delta_1, \delta_2}((d_2 d_1)(x))y + \varepsilon_{\delta_1 + \delta_2, \xi} x((d_1 d_2)(y)) - \varepsilon_{\delta_1, \delta_2} \varepsilon_{\delta_1 + \delta_2, \xi} x((d_2 d_1)(y))
that is, writing d=[d1,d2]εd = [d_1, d_2]_\varepsilon and δ=δ1+δ2\delta = \delta_1 + \delta_2,
d(xy)=(dx)y+εδ,ξx(dy) d(xy) = (dx)y + \varepsilon_{\delta, \xi} x(dy)
which proves that dd is an ε\varepsilon-derivation.

On the other hand, if, in (11), we let d1=d2=dd_1 = d_2 = d, δ1=δ2=δ\delta_1 = \delta_2 = \delta and εδ,δ=−1\varepsilon_{\delta, \delta} = -1, we obtain, since then εδ,δ+ξ=−εδ,ξ\varepsilon_{\delta, \delta + \xi} = -\varepsilon_{\delta, \xi} by (1),

d2(xy)=(d2x)y+ε2δ,ξx(d2y) d^2(xy) = (d^2 x)y + \varepsilon_{2\delta, \xi} x(d^2 y)
and as ε2δ,ξ=1\varepsilon_{2\delta, \xi} = 1 it is seen that d2d^2 is a derivation.

Bourbaki puts the proof directly after the statement, so what is above is the statement and its proof together.

Cited by

Cites

Nothing.

Transcribed from the printed edition, 1998, Springer. Not translated.