In algebra, a purely inseparable extension of fields is an extension k ⊆ K of fields of characteristic p > 0 such that every element of K is a root of an equation of the form xq = a, with q a power of p and a in k. Purely inseparable extensions are sometimes called radicial extensions, which should not be confused with the similar-sounding but more general notion of radical extensions.
E\supseteqF
\alpha\inE\setminusF
\alpha
F\supseteqF
Several equivalent and more concrete definitions for the notion of a purely inseparable extension are known. If
E\supseteqF
\alpha\inE
n\geq0
pn | |
\alpha |
\inF
pn | |
X |
-a
n\geq0
a\inF
It follows from the above equivalent characterizations that if
E=F[\alpha]
pn | |
\alpha |
\inF
n\geq0
pn | |
x |
\inF
n\geq0
\alpha
E\supseteqF
If F is an imperfect field of prime characteristic p, choose
a\inF
\alpha
f(\alpha)=0
\alphap=a
F[\alpha]\supseteqF
E=F[\alpha]
E\supseteqF
Purely inseparable extensions do occur naturally; for example, they occur in algebraic geometry over fields of prime characteristic. If K is a field of characteristic p, and if V is an algebraic variety over K of dimension greater than zero, the function field K(V) is a purely inseparable extension over the subfield K(V)p of pth powers (this follows from condition 2 above). Such extensions occur in the context of multiplication by p on an elliptic curve over a finite field of characteristic p.
E\supseteqF
F\subseteqK\subseteqE
F\subseteqK\subseteqE
F\subseteqK
K\subseteqE
E\supseteqF
\alpha\inE\setminusF
\alpha
E\supseteqF
E\supseteqF
K=Fix(Gal(E/F))
introduced a variation of Galois theory for purely inseparable extensions of exponent 1, where the Galois groups of field automorphisms in Galois theory are replaced by restricted Lie algebras of derivations. The simplest case is for finite index purely inseparable extensions K⊆L of exponent at most 1 (meaning that the pth power of every element of L is in K). In this case the Lie algebra of K-derivations of L is a restricted Lie algebra that is also a vector space of dimension n over L, where [''L'':''K''] = pn, and the intermediate fields in L containing K correspond to the restricted Lie subalgebras of this Lie algebra that are vector spaces over L. Although the Lie algebra of derivations is a vector space over L, it is not in general a Lie algebra over L, but is a Lie algebra over K of dimension n[''L'':''K''] = npn.
A purely inseparable extension is called a modular extension if it is a tensor product of simple extensions, so in particular every extension of exponent 1 is modular, but there are non-modular extensions of exponent 2 . and gave an extension of the Galois correspondence to modular purely inseparable extensions, where derivations are replaced by higher derivations.