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Degree Of A Field Extension





DEFINITION AND NOTATION


Suppose that ''E''/''F'' is a Field Extension . Then ''E'' may be considered as a Vector Space over ''F'' (the field of scalars). The Dimension of this vector space is called the degree of the field extension, and it is denoted by {Link without Title} .

The degree may be finite or infinite, the field being called a finite extension or '''infinite extension''' accordingly. An extension ''E''/''F'' is also sometimes said to be simply '''finite''' if it is a finite extension; this should not be confused with the fields themselves being Finite Field s (fields with finitely many elements).

The degree should not be confused with the Transcendence Degree of a field; for example, the field Q(''X'') of Rational Function s has infinite degree over Q, but transcendence degree only equal to 1.


THE MULTIPLICITIVITY FORMULA FOR DEGREES


Given three fields arranged in a tower, say ''K'' a subfield of ''L'' which is in turn a subfield of ''M'', there is a simple relation between the degrees of the three extensions ''L''/''K'', ''M''/''L'' and ''M''/''K'':
: = [M:L \cdot [L:K].
In other words, the degree going from the "bottom" to the "top" field is just the product of the degrees going from the "bottom" to the "middle" and then from the "middle" to the "top". It is quite analogous to Lagrange's Theorem in Group Theory , which relates the order of a group to the order and index of a subgroup — indeed Galois Theory shows that this analogy is more than just a coincidence.

The formula holds for both finite and infinite degree extensions. In the infinite case, the product is interpreted in the sense of products of Cardinal Number s. In particular, this means that if ''M''/''K'' is finite, then both ''M''/''L'' and ''L''/''K'' are finite.

If ''M''/''K'' is finite, then the formula imposes strong restrictions on the kinds of fields that can occur between ''M'' and ''K'', via simple arithmetical considerations. For example, if the degree is a Prime Number ''p'', then for any intermediate field ''L'', one of two things can happen: either [''M'':''L'' = ''p'' and = 1, in which case ''L'' is equal to ''K'', or [''M'':''L'' = 1 and [''L'':''K''] = ''p'', in which case ''L'' is equal to ''K''. Therefore there are no intermediate fields (apart from ''M'' and ''K'' themselves).


Proof of the multiplicitivity formula in the finite case


Suppose that ''K'', ''L'' and ''M'' form a tower of fields as in the degree formula above, and that both ''d'' = and ''e'' = [''M'':''L'' are finite. This means that we may select a Basis {''u''1, ..., ''u''''d''} for ''L'' over ''K'', and a basis {''w''1, ..., ''w''''e''} for ''M'' over ''L''. We will show that the elements ''u''''m''''w''''n'', for ''m'' ranging through 1, 2, ..., ''d'' and ''n'' ranging through 1, 2, ..., ''e'', form a basis for ''M''/''K''; since there are precisely ''de'' of them, this proves that the dimension of ''M''/''K'' is ''de'', which is the desired result.

First we check that they Span ''M''/''K''. If ''x'' is any element of ''M'', then since the ''w''''n'' form a basis for ''M'' over ''L'', we can find elements ''a''''n'' in ''L'' such that
: x = \sum_{n=1}^e a_n w_n = a_1 w_1 + \cdots + a_e w_e.
Then, since the ''u''''m'' form a basis for ''L'' over ''K'', we can find elements ''b''''m'',''n'' in ''K'' such that for each ''n'',
: a_n = \sum_{m=1}^d b_{m,n} u_m = b_{1,n} u_1 + \cdots + b_{d,n} u_d.
Then using the Distributive Law and Associativity of multiplication in ''M'' we have
: x = \sum_{n=1}^e \left(\sum_{m=1}^d b_{m,n} u_m ight) w_n = \sum_{n=1}^e \sum_{m=1}^d b_{m,n} (u_m w_n),
which shows that ''x'' is a linear combination of the ''u''''m''''w''''n'' with coefficients from ''K''; in other words they span ''M'' over ''K''.

Secondly we must check that they are Linearly Independent over ''K''. So assume that
: 0 = \sum_{n=1}^e \sum_{m=1}^d b_{m,n} (u_m w_n)
for some coefficients ''b''''m'',''n'' in ''K''. Using distributivity and associativity again, we can group the terms as
: 0 = \sum_{n=1}^e \left(\sum_{m=1}^d b_{m,n} u_m ight) w_n,
and we see that the terms in parentheses must be zero, because they are elements of ''L'', and the ''w''''n'' are linearly independent over ''L''. That is,
: 0 = \sum_{m=1}^d b_{m,n} u_m
for each ''n''. Then, since the ''b''''m'',''n'' coefficients are in ''K'', and the ''u''''m'' are linearly independent over ''K'', we must have that ''b''''m'',''n'' = 0 for all ''m'' and all ''n''. This shows that the elements ''u''''m''''w''''n'' are linearly independent over ''K''. This concludes the proof.


Proof of the formula in the infinite case


In this case, we start with bases ''u''α and ''w''β of ''L''/''K'' and ''M''/''L'' respectively, where α is taken from an indexing set ''A'', and β from an indexing set ''B''. Using an entirely similar argument as the one above, we find that the products ''u''α''w''β form a basis for ''M''/''K''. These are indexed by the Cartesian Product ''A'' × ''B'', which by definition has Cardinality equal to the product of the cardinalities of ''A'' and ''B''.


EXAMPLES




GENERALIZATION


Given two Skew Field s (division rings) ''E'' and ''F'' with ''F'' contained in ''E'' and the multiplication and addition of ''F'' being the restriction of the operations in ''E'', we can consider ''E'' as a vector space over ''F'' in two ways: having the scalars act on the left, giving a dimension and having them act on the right, giving a dimension [''E'':''F'' r. The two dimensions need not agree. Both dimensions however satisfy a multiplication formula for towers of skew fields; the proof above applies to left-acting scalars without change.


REFERENCES


  • page 215, 1 Proof of the multiplicitivity formula.

  • page 465, 2 Briefly discusses the infinite dimensional case.