Differential Forms
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Differential Forms

Henri Cartan

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eBook - ePub

Differential Forms

Henri Cartan

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About This Book

`Cartan's work provides a superb text for an undergraduate course in advanced calculus, but at the same time it furnishes the reader with an excellent foundation for global and nonlinear algebra.`—Mathematical Review
`Brilliantly successful.`—Bulletin de l'Association des Professeurs de Mathematiques
`The presentation is precise and detailed, the style lucid and almost conversational . . . clearly an outstanding text and work of reference.`—Annales
Cartan's Formes Differentielles was first published in France in 1967. It was based on the world-famous teacher's experience at the Faculty of Sciences in Paris, where his reputation as an outstanding exponent of the Bourbaki school of mathematics was first established.
Addressed to second- and third-year students of mathematics, the material skillfully spans the pure and applied branches in the familiar French manner, so that the applied aspects gain in rigor while the pure mathematics loses none of its dignity. This book is equally essential as a course text, as a work of reference, or simply as a brilliant mathematical exercise.

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Year
2012
ISBN
9780486139111

Chapter 1

Differential forms

1. Multilinear alternating mappings

1.1 Definition of an alternating multilinear mapping

Much of the following will be of interest purely from the point of view of that division of algebra which is concerned with the study of vector spaces over an arbitrary commutative field K (no restriction being placed on the characteristic of the field). However, we shall confine ourselves in exposition to normed vector spaces over the fields R or C: to illustrate, let us take R.
Suppose then that E, F are two normed vector spaces. We have already considered (Chap. 1, § 1.8, Differential Calculus) the normed vector space
e9780486139111_img_8466.gif
p(E; F) of the p-linear continuous mappings Ep → F; for p = 1 we write for simplicity
e9780486139111_img_8466.gif
(E;
F); for p = 0 we define
e9780486139111_img_8466.gif
0(E; F) = F. We also considered the vector subspace of
e9780486139111_img_8466.gif
p(E; F) formed by the p-linear symmetric mappings. We shall now introduce a second subspace
e9780486139111_i0002.webp
of
e9780486139111_img_8466.gif
p(E; F).
DEFINITION. A mapping f
e9780486139111_img_8466.gif
p(E; F) is called alternating if its value f(x1, ..., xp) is null whenever xi = xi+1 for at least one i (1 ≤ i < p). (We agree that for p = 1 every linear function E → F is an alternation.)
It is evident that the p-linear alternating mappings form a vector subspace of
e9780486139111_img_8466.gif
p(E; F); we denote it by
e9780486139111_i0003.webp
Then
e9780486139111_i0004.webp
; by definition we put
e9780486139111_i0005.webp
The vector subspace
e9780486139111_i0006.webp
is closed in
e9780486139111_img_8466.gif
P(E; F) ; indeed, suppose f ∈
e9780486139111_img_8466.gif
p(E; F) is the limit of a sequence fn
e9780486139111_i0007.webp
: then limn→∞ || f
e9780486139111_img_8210.gif
fn || = 0; a fortiori, for x1, . . ., xp ∈ E, the limit of ƒn(x1, ..., xp) is ƒ(x1, ... , xp). Thus if xi = xi+1, it follows that
e9780486139111_i0008.webp
Q.E.D.
Before stating further properties of multilinear alternating mappings we require a few preliminaries concerning permutation groups.

1.2 Permutation groups

Let
e9780486139111_img_8721.gif
p denote th...

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