Pierre Pansu
Centre national de la recherche scientifique
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Archive | 1984
Marcel Berger; Pierre Pansu; Jean-Pic Berry; Xavier Saint-Raymond
We fix an n-dimensional Euclidean space E, and denote by Q ( E ) the space of affine quadratic forms q over E; (overrightarrow q ), an element of Q ((overrightarrow E )), will be the symbol of q. A sphere is given by a form q, written as n n
Archive | 1984
Marcel Berger; Pierre Pansu; Jean-Pic Berry; Xavier Saint-Raymond
Archive | 1984
Marcel Berger; Pierre Pansu; Jean-Pic Berry; Xavier Saint-Raymond
q = k{left| {left. cdot right|} right.^2} + (alpha left| cdot right.) + h, where alpha in overrightarrow E and k, h in R;
Archive | 1984
Marcel Berger; Pierre Pansu; Jean-Pic Berry; Xavier Saint-Raymond
Archive | 1984
Marcel Berger; Pierre Pansu; Jean-Pic Berry; Xavier Saint-Raymond
n nit is an actual sphere if k ≠ 0 and ‖α‖2 > 4kh; if k ≠ 0 and ‖α‖2 = 4kh the image is a single point (sphere of zero radius), and if ‖α‖2 < 4kh the image is empty, and we say that q represents a sphere “of imaginary radius”. For k = 0, h ≠ 0, we obtain a hyperplane (if α ≠ 0); the case k = 0 and α = 0, h ≠ 0 represents the point at infinity of E.
Archive | 1984
Marcel Berger; Pierre Pansu; Jean-Pic Berry; Xavier Saint-Raymond
We’ll be working in a d-dimensional real affine space X, for d finite. A polytope is a convex compact set with non-empty interior, which can be realized as the intersection of a finite number of closed half-spaces of X (cf. 2.G). We shall assume there are no superfluous half-spaces in the intersection. For d = 2 we use the word polygon.
Archive | 1984
Marcel Berger; Pierre Pansu; Jean-Pic Berry; Xavier Saint-Raymond
We have shown, at the beginning of chapter 4 why it is necessary to go beyond the framework of affine spaces, adjoining to them points at infinity This is now possible in the following way: we associate to the affine space X its universal space ( hat X) (cf. 3.D), which is a vector space in which X is embedded as an affine hyperplane whose direction is a vector hyperplane of (hat X). Considering now the projectivization (tilde X = Pleft( {hat X} right)) , we see that (tilde X) is the disjoint union of two sets: P( X), which is canonically identified with X, and P ((vec X)), which, being the space of lines in (vec X), is also the space of directions of lines in X. We denote it by ({infty _X} = Pleft( {vec X} right)) We write ( tilde X = X cup {infty _X}), and say that ∞x is the hyperplane at infinity in X.
Archive | 1984
Marcel Berger; Pierre Pansu; Jean-Pic Berry; Xavier Saint-Raymond
To any four distinct points (a i ) i = 1,2,3,4 on a projective line (considered by itself or inside a projective space), we associate a scalar, denoted by [a i ] = [a l, a 2, a 3, a 4], and called the cross-ratio of these four points. For points on an affine line D, the cross-ratio is defined to be the same as on the completion (tilde D = D cup {infty _D}) (cf. 5.A).
Archive | 1984
Marcel Berger; Pierre Pansu; Jean-Pic Berry; Xavier Saint-Raymond
The sphere is a compact connected topological space; for d ≥ 2, it is also simply connected, which means that every closed curve in S can be deformed into a point (such is not the case for either S 1 or P n (R)).
Archive | 2004
Peter Winkler; Edward J. Barbeau; Marcel Berger; Pierre Pansu; Jean-Pic Berry; Xavier Saint-Raymond; George W. Bluman; T. Cacoullos; Tomasz Zastawniak; David W. Cohen
Let X be a set; we denote by S X the set of all bijections (permutations) f: X → X from X into itself, and we endow S X with the law of composition given by (f, g) ↦ f ° g. Thus S X becomes a group, called the permutation group or symmetric group of X.