Bourbaki

Proposition 5

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

Algebra, chapter III, § 10. Derivations

Suppose that A\mathbf{A} is an integral domain and let L\mathbf{L} be its field of fractions. Every derivation of A\mathbf{A} into a vector space E\mathbf{E} over L\mathbf{L} (considered as an A\mathbf{A}-module) can be extended uniquely to a derivation of L\mathbf{L} into E\mathbf{E}.

Let dd be a derivation of A\mathbf{A} into E\mathbf{E} and dˉ\bar{d} a derivation of L\mathbf{L} into E\mathbf{E} extending dd; then, for u∈A,v∈A,v≠0u \in \mathbf{A}, v \in \mathbf{A}, v \neq 0, of necessity, by virtue of (19),

dˉ(u/v)=v−1du−uv−2dv \bar{d}(u/v) = v^{-1}du - uv^{-2}dv
which proves the uniqueness of dˉ\bar{d}. Conversely, we show that dˉ\bar{d} can be defined by formula (20); it must first be verified that if u/v=u′/v′u/v = u'/v' the value of the right hand side of (20) does not change when uu is replaced by u′u' and vv by v′v'. Now, uv′=vu′uv' = vu', hence v′(du)+u(dv′)=v(du′)+u′(dv)v'(du) + u(dv') = v(du') + u'(dv) and therefore v′(du−uv−1dv)=v(du′−u′v′−1dv′)v'(du - uv^{-1}dv) = v(du' - u'{v'}^{-1}dv'), since uv′v−1=u′uv'v^{-1} = u' and u′v′−1v=uu'{v'}^{-1}v = u. Thus a mapping dˉ:L→E\bar{d}: \mathbf{L} \to \mathbf{E} has been defined which extends dd; it is immediately verified that it is K\mathbf{K}-linear and a derivation.

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

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Cites

Nothing.

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