Simplicity of an algebraic extension
Let
Proof
Suppose
is simple and algebraic over πΉ = πΎ ( πΌ ) , so that πΎ is the minimal polynomial for π πΎ ( π₯ ) β πΎ [ π₯ ] . If πΌ is an intermediate field, then πΈ is also simple and algebraic over πΉ = πΈ ( πΌ ) , so that πΈ is the minimal polynomial. Moreover, π πΈ ( π₯ ) β πΈ [ π₯ ] is a factor of π πΈ ( π₯ ) . π πΎ ( π₯ )
will turn out to completely determine the intermediate field π πΈ ( π₯ ) , and since πΈ only has finitely many factors in π πΎ ( π₯ ) , this proves the forward direction. In fact, ββ πΎ [ π₯ ] will be generated over πΈ by the coΓ«fficients of πΎ . π πΈ ( π₯ ) To show this, let
be the subfield of πΈ β² generated by the coΓ«fficients and πΈ . Then πΎ , and since π πΈ ( π₯ ) β πΈ β² [ π₯ ] is irreducible in the extension field π πΈ ( π₯ ) , so too is it irreducible in πΈ β² . Since πΈ β² and πΈ β² ( πΌ ) = πΉ = πΈ ( πΌ ) , it follows (see tower of field extensions) πΉ : πΈ : πΈ β² : πΎ d e g β‘ π πΈ = [ πΉ : πΈ β² ] = [ πΉ : πΈ ] [ πΈ : πΈ β² ] = d e g β‘ π πΈ [ πΈ : πΈ β² ] , so
, i.e. [ πΈ : πΈ β² ] = 1 , as required. πΈ = πΈ β² For the converse, assume that there are only finitely many intermediate fields
. The extension πΉ : πΈ : πΎ must be finitely generated, for otherwise the infinite sequence of subextensions πΉ : πΎ πΎ βͺ πΎ ( πΌ 1 ) βͺ πΎ ( πΌ 2 ) βͺ β― βͺ πΉ would give infinitely many intermediate fields. If
is a Galois field so is πΎ , and then by Finite extension of a Galois field πΉ is simple. πΉ : πΎ Let us consider the case
is infinite, where we need to show that every finitely generated algebraic extension πΎ is simple. πΉ = πΎ ( πΌ 1 , β¦ , πΌ π ) Arguing inductively, we may assume w.l.o.g. that
. For every πΉ = πΎ ( πΌ , π½ ) , we have the intermediate field π β πΎ πΎ ( πΌ , π½ ) : πΎ ( π πΌ + π½ ) : πΎ . But there are only finitely many such intermediate extensions. Since
is infinite, we must have πΎ πΎ ( π β² πΌ + π½ ) = πΎ ( π πΌ + π½ ) for some
in π β² β π , whence πΎ πΌ = ( π β² πΌ + π½ ) β ( π πΌ + π½ ) π β² β π β πΎ ( πΆ πΌ + π½ ) , π½ = ( π πΌ + π½ ) β π πΌ β πΎ ( π πΌ + π½ ) ; so
. Thus πΎ ( πΌ , π½ ) β πΎ ( π πΌ + π½ ) , and we are done. πΎ ( π πΌ + π½ ) = πΎ ( πΌ , π½ )