Galois Theory
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Galois Theory

Lectures Delivered at the University of Notre Dame by Emil Artin (Notre Dame Mathematical Lectures,

Emil Artin, Arthur N. Milgram, Arthur N. Milgram

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eBook - ePub

Galois Theory

Lectures Delivered at the University of Notre Dame by Emil Artin (Notre Dame Mathematical Lectures,

Emil Artin, Arthur N. Milgram, Arthur N. Milgram

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About This Book

In the nineteenth century, French mathematician Evariste Galois developed the Galois theory of groups-one of the most penetrating concepts in modem mathematics. The elements of the theory are clearly presented in this second, revised edition of a volume of lectures delivered by noted mathematician Emil Artin. The book has been edited by Dr. Arthur N. Milgram, who has also supplemented the work with a Section on Applications.
The first section deals with linear algebra, including fields, vector spaces, homogeneous linear equations, determinants, and other topics. A second section considers extension fields, polynomials, algebraic elements, splitting fields, group characters, normal extensions, roots of unity, Noether equations, Jummer's fields, and more.
Dr. Milgram's section on applications discusses solvable groups, permutation groups, solution of equations by radicals, and other concepts.

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Information

Year
2012
ISBN
9780486158259

II FIELD THEORY

A. Extension Fields.

If E is a field and F a subset of E which, under the operations of addition and multiplication in E, itself forms a field, that is, if F is a subfield of E, then we shall call E an extension of F. The relation of being an extension of F will be briefly designated by F ⊂ E. If α, ÎČ, Îł, ... are elements of E, then by F(α, ÎČ, Îł, ...) we shall mean the set of elements in E which can be expressed as quotients of polynomials in α, ÎČ, Îł,... with coefficients in F. It is clear that
F(α, ÎČ, Îł,...) is a field and is the smallest extension of F which contains the elements α, ÎČ, Îł, ... . We shall call F(α, ÎČ, Îł,...) the field obtained after the adjunction of the elements α, ÎČ, Îł,... to F, or the field generated out of F by the elements α, ÎČ, Îł,... In the sequel all fields will be assumed commutative.
If F ⊂ E, then ignoring the operation of multiplication defined between the elements of E, we may consider E as a vector space over F. By the degree of E over F, written (E/F), we shall mean the dimension of the vector space E over F. If (E/F) is finite, E will be called a finite extension.
THEOREM 6. If F, B, E are three fields such that F ⊂ B ⊂ E, then
(E/F) (B/F)(E/B).
Let A1 , A2, ..., Ar be elements of E which are linearly independent with respect to B and let C1, C2,..., Cs be elements of B which are independent with respect to F. Then the products Ci Aj where i = 1, 2, ... , s and j = 1, 2, ... , r are elements of E which are independent with respect to F. For if
e9780486158259_i0058.webp
, then
e9780486158259_i0059.webp
is a linear combination of the Aj with coefficients in B and because the A, were independent with respect to B we have
e9780486158259_i0060.webp
for each j. The independence of the C, with respect to F then requires that each aij = 0. Since there are r ‱ s elements CiAj we have shown that for each r ≀ ( E/B ) and s ≀ ( B/F ) the degree ( E/F ) ≄ r
e9780486158259_img_8729.gif
s. Therefore, ( E/F ) ≄ (B/F) (E/B). If one of the latter numbers is infinite, the theorem follows. If both ( E/B ) and ( B/F ) are finite, say r and s respectively, we may suppose that the Aj and the Ci are generating systems of E and B respectively, and we show that the set of products Ci Aj is a generating system of E over F. Each A
e9780486158259_img_8714.gif
E can be expressed linearly in terms of the Aj with coefficients in B. Thus, A =
e9780486158259_img_8721.gif
Bj Aj. Moreover, each Bj being an element of B can be expressed linearly with coefficients in F in terms of the Ci, i.e., Bj =
e9780486158259_img_8721.gif
aij Ci, j = 1, 2, ... , r. Thus, A =
e9780486158259_img_8721.gif
aij CiAj and the CiAj form an independent generating system of E over F.
e9780486158259_i0061.webp

B. Polynomials.

An expression of the form aoxn + a1xn–1+ ... + an is called a polynomial in F of degree n if the coefficients ao, ... , an are elements of the field F and ao ≠0. Multiplication and addition of polynomials are performed in the usual way3.
A polynomial in F is called reducible in F if it is equal to the product of two polynomials in F each of degree at least one. Polynomials which are not reducible in F are called irreducible in F.
If f(x) = g (x)
e9780486158259_img_8729.gif
h(x) is a relation which holds between the polynomials f (x), g (x), h (x) in a field F, then we shall say that g (x) divides f(x) in F, or that g (x) is a factor of f (x). It is readily seen ...

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