Fundamentals of Advanced Mathematics 3
Differential Calculus, Tensor Calculus, Differential Geometry, Global Analysis
Henri Bourls
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First published 2019 in Great Britain and the United States by ISTE Press Ltd and Elsevier Ltd
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ISBN 978-1-78548-250-2
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Preface
Henri Bourls June 2019
This third volume of of this third volume. Nonetheless, we will need to consider a few generalizations to sketch the so-called convenient context for more recent developments in global analysis; more on this later. We will also present the Carathdory conditions, which are finer than the classical CauchyLipschitz existence and uniqueness conditions for solutions of finite-dimensional ordinary differential equations.
Global questions demand another perspective. Seen through our window, the Earth appears entirely flat, yet even the Greeks in the age of Plato knew better, as testified by an excerpt from his Phaedo (108, e). Knowledge of the Earths shape undoubtedly extended back to the Pythagoreans in the 6th Century BC. Thus, Euclid, who was an avid student of Platos work (consider, for example, his construction of the five Platonic solids in Book XIII of the Elements ), certainly also knew that the Earth is round. Yet his geometry is quite different from the geometry of a sphere. Euclidean geometry offers a good local approximation of spherical geometry but was of course useless for the lengthy voyages of the Renaissance. Global analysis must therefore be expressed in the framework of manifolds , a concept which generalizes curves and surfaces since Riemann.
Ever since the invention of variational calculus in the late 17th Century, it has become common in mathematics to argue about sets of functions. If certain conditions are satisfied, these sets can be endowed with the structure of a manifold, in which case they are called functional manifolds and imagined as deformed versions of the usual function spaces (in the same way that the Earth might be imagined as a deformed version of the plane). Banach manifolds were the first candidates to be considered as a framework for global analysis in the late 1950s and the 1960s [ will demonstrate the considerable value of this approach.
, alongside the theory of differential p -forms.
Our formalism first begins to truly bear fruit in ).
Lie groups are manifolds but also groups; in .
On a reductive Lie group G , we can also fully develop the theory of harmonic analysis (Fourier transforms of functions or tempered distributions). The abelian case will be presented in detail: when G=n , we recover the usual notion of Fourier transform; when G is the torus Tn , we recover the Fourier series expansion of periodic functions or distributions. The non-abelian case would fill another entire volume and thus will only be briefly mentioned (even though engineering applications have recently been found ].
Defining a geometry on a manifold is equivalent to equipping this manifold with a connection (, Appendix II), who hoped to find a way to unify the theories of gravitation and electromagnetism.
See the Wikipedia article on CoxeterDynkin diagrams.
Errata for Volume 1 and Volume 2
Volume 1 (Contd)
- 1) On p. 12, the fifth line of (V) should read R instead of R .
- 2) On p. 22, on the right-hand side of , it should read lim instead of lim .
- 3) On p. 41, line 10 should read the cardinal of G / H (equal to the cardinal of G \ H ) instead of this cardinal.
- 4) On p. 45, the first line after should read M 3 instead of G .
- 5) On p. 190, in Definition 3.177, it should read n instead of n .
- 6) On p. 191, in the first line after [3.70], add also denoted as d p after operator.
- 7) On p. 193, line 17 should read Sp instead of Sn .
- 8) On p. 220, line 7 should read = j J j where the elementary divisors j are pairwise non-associated and maximal powers (among all elementary divisors) of irreducible polynomials instead of = i = 1 n i .
Volume 2
- 1) On p. 12, line 6 should read K () instead of K ().
- 2) On p. 17, line 19 should read instead of =; line 21 should read does not exist instead of exists.
- 3) On p. 20, line 11 should read 0 i r instead of 1 i r .
- 4) On p. 24, line 28 should read xK