Bourbaki

Theorem 4

Tag 06V4, permanent. Cite it as [Bourbaki, Tag 06V4].

Algebra, V, p. 133, § 16. Differential criteria of separability

Let P be a perfect field, L an extension of P and K a subextension of L; we suppose that L is a finitely generated extension of K. Then the canonical L-linear mapping a:Ωp(K)⊗KL→Ωp(L)a : \Omega_p(K) \otimes_K L \to \Omega_p(L) has index equal to the transcendence degree of L over K.

If EE and FF are two subextensions of LL such that E⊂FE \subset F, we denote by α(F/E)\alpha(F/E) the canonical FF-linear mapping of Ωp(E)⊗EF\Omega_p(E) \otimes_E F into Ωp(F)\Omega_p(F) and when it is defined, the index of α(F/E)\alpha(F/E) will be written d(F/E)d(F/E). If E,FE, F and GG are three subextensions of LL such that E⊂F⊂GE \subset F \subset G, we have a commutative diagram

Ωp(F)⊗FG→α(G/F)Ωp(G)↑α(F/E)⊗FIdG↑α(G/E)(Ωp(E)⊗EF)⊗FG→βΩp(E)⊗EG \begin{array}{ccc} \Omega_p(F) \otimes_F G & \xrightarrow{\alpha(G/F)} & \Omega_p(G) \\ \uparrow \alpha(F/E) \otimes_F \mathrm{Id}_G & & \uparrow \alpha(G/E) \\ (\Omega_p(E) \otimes_E F) \otimes_F G & \xrightarrow{\beta} & \Omega_p(E) \otimes_E G \end{array}

where β\beta is the canonical isomorphism defined in Prop. 2 (II, p. 278). Since the index is clearly invariant under extension by scalars and the index of an isomorphism is zero, Lemma 2 (VV, p. 133) shows that the index d(G/E)d(G/E) is defined when d(F/E)d(F/E) and d(G/F)d(G/F) are and then

d(G/E)=d(G/F)+d(F/E). d(G/E) = d(G/F) + d(F/E).

Since LL is a finitely generated extension of KK, Formula (5) and the Cor. of VV, p. 111 shows that it is enough to consider the case where xx exists such that L=K(x)L = K(x); further if xx is algebraic over KK, there exists a power qq of the characteristic exponent of LL such that xqx^q is separable algebraic over KK (VV, p. 44, Prop. 13). So it is enough to establish the equality d(L/K)=tr⁡.deg⁡KLd(L/K) = \operatorname{tr} . \deg_K L in the three special cases below:

a) xx is transcendental over KK: then aa is injective and its cokernel is of rank 1 over LL (VV, p. 129, Cor.) ; so we have d(L/K)=1d(L/K) = 1 and also tr⁡.deg⁡KL=1\operatorname{tr} . \deg_K L = 1.

b) xx is separable algebraic over KK: then aa is bijective (VV, p. 130, Cor. 2), whence d(L/K)=0d(L/K) = 0; clearly also tr⁡.deg⁡KL=0\operatorname{tr} . \deg_K L = 0.

c) The field LL is of characteristic p≠0p \neq 0, x∉Kx \notin K and xp=ax^p = a is in KK: the cokernel CC of aa is isomorphic to ΩK(L)\Omega_K(L), and since {x}\{ x \} is a pp-basis of LL over KK, the space CC is of dimension 1 over LL (VV, p. 102, Th. 1). Since aa is a pp-th power in LL, we have dL/pa=0d_{L/pa} = 0 and the kernel of aa contains the subspace RR of U=Ωp(K)⊗KLU = \Omega_p(K) \otimes_K L generated by dK/pa⊗1d_{K/pa} \otimes 1. For each y∈Ky \in K let Δ(y)\Delta(y) be the residue class of dK/py⊗1d_{K/p}y \otimes 1 mod RR; then AA is a PP-derivation of KK into U/RU/R such that Δ(a)=0\Delta(a) = 0. Prop. 5 (VV, p. 101) shows that AA extends to a PP-derivation DD of LL into U/RU/R. Hence there exists an LL-linear mapping β:Ωp(L)→U/R\beta : \Omega_p(L) \to U/R such that D=β∘dL/PD = \beta \circ d_{L/P} and β∘a\beta \circ a is the canonical mapping of UU onto U/RU/R. This proves RR to be the kernel of aa. Since PP is perfect, we have P(KP)=KpP(K^P) = K^p, whence a∉P(KP)a \notin P(K^P) and finally dK/pa≠0d_{K/pa} \neq 0 (VV, p. 103, Prop. 6). The kernel and cokernel of aa are thus of dimension 1, whence d(L/K)=0d(L/K) = 0, and we also have tr⁡.deg⁡KL=0\operatorname{tr} . \deg_K L = 0.

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

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Transcribed from the printed edition, 2003, Springer. Not translated.