let F be Field; for E being FieldExtension of F
for a being Element of E st not a in F & a ^2 in F holds
( {(1. E),a} is Basis of (VecSp ((FAdj (F,{a})),F)) & deg ((FAdj (F,{a})),F) = 2 )
let E be FieldExtension of F; for a being Element of E st not a in F & a ^2 in F holds
( {(1. E),a} is Basis of (VecSp ((FAdj (F,{a})),F)) & deg ((FAdj (F,{a})),F) = 2 )
let a be Element of E; ( not a in F & a ^2 in F implies ( {(1. E),a} is Basis of (VecSp ((FAdj (F,{a})),F)) & deg ((FAdj (F,{a})),F) = 2 ) )
assume AS:
( not a in F & a ^2 in F )
; ( {(1. E),a} is Basis of (VecSp ((FAdj (F,{a})),F)) & deg ((FAdj (F,{a})),F) = 2 )
reconsider a1 = a as F -algebraic Element of E by AS, lemBas0;
reconsider b = a ^2 as Element of F by AS;
B: deg (MinPoly (a1,F)) =
deg (X^2- b)
by AS, lemBas1
.=
2
by FIELD_9:def 4
;
Base a1 = {(1. E),a}
hence
{(1. E),a} is Basis of (VecSp ((FAdj (F,{a})),F))
by FIELD_6:65; deg ((FAdj (F,{a})),F) = 2
thus
deg ((FAdj (F,{a})),F) = 2
by B, FIELD_6:67; verum