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Showing papers on "Frame bundle published in 1987"


Journal Article
TL;DR: In this paper, the conditions générales d'utilisation (http://www.compositio.org/conditions) of the agreement with the Foundation Compositio Mathematica are described.
Abstract: © Foundation Compositio Mathematica, 1987, tous droits réservés. L’accès aux archives de la revue « Compositio Mathematica » (http: //http://www.compositio.nl/) implique l’accord avec les conditions générales d’utilisation (http://www.numdam.org/conditions). Toute utilisation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright.

74 citations



Journal ArticleDOI
TL;DR: In this paper, a new derivation of the curvature formula (−26/12m3+1/6m)δn, −m for the canonical holomorphic line bundle over DiffS1/S1 is given which clarifies the relation of that bundle with the complex line bundles over infinite-dimensional Grassmannians.
Abstract: The recent results by Bowick and Rajeev on the relation of the geometry of DiffS1/S1 and string quantization in ℝd are extended to a string moving on a group manifold. A new derivation of the curvature formula (−26/12m3+1/6m)δn, −m for the canonical holomorphic line bundle over DiffS1/S1 is given which clarifies the relation of that bundle with the complex line bundles over infinite-dimensional Grassmannians, studied by Pressley and Segal.

41 citations


Journal ArticleDOI
TL;DR: In this paper, a compact K/ihler manifold of dimension n with a K-ihler form and a holomorphic vector bundle over the manifold is considered and its curvature is denoted by R, where R is the contraction of R with respect to the metric 4.
Abstract: Let M be a compact K/ihler manifold of dimension n with a K/ihler form and let g be a holomorphic vector bundle over M. A Hermitian metric on g gives rise to a natural choice of connection and its curvature is denoted by R. Let K be the contraction of R with respect to the metric 4. Locally, if X1, ..., X, is a unitary frame (for the holomorphic tangent bundle of M) at a point, then K is the mean curvature

30 citations



Journal ArticleDOI
TL;DR: In this paper, a new approach to gauge fields on a discrete space-time is proposed, in which the fundamental object is a discrete version of a principal fibre bundle and if the bundle is twisted, the gauge fields are topologically non-trivial automatically.
Abstract: A new approach to gauge fields on a discrete space-time is proposed, in which the fundamental object is a discrete version of a principal fibre bundle. If the bundle is twisted, the gauge fields are topologically non-trivial automatically.

27 citations


Journal ArticleDOI
01 Feb 1987
TL;DR: In this article, it was shown that any vector bundle E over a compact base manifold admits a complete metric of negative (respectively non-positive) curvature provided M admits a metric of positive (non-negative) curvatures.
Abstract: It is shown that any vector bundle E over a compact base manifold M admits a complete metric of negative (respectively nonpositive) curvature provided M admits a metric of negative (nonpositive) curvature.

19 citations


Journal ArticleDOI
TL;DR: In this paper, it was shown that the cotangent bundle T ∗ T M of the tangent bundle of any differentiable manifold M carries an integrable almost tangent structure which is generated by a natural lifting procedure from the canonical almost-tent structure (vertical endomorphism) of T M.

17 citations


Journal ArticleDOI
TL;DR: In this paper, it was shown that for any rational surface, the existence of simple vector bundles is irreducible under certain assumptions on the moduli scheme of H-stable vector bundles of rank r, c 1, c 2 with first Chern class c a and second Chern classc 2.
Abstract: Let S be a smooth, connected, projective surface (over ~) and H an ample divisor on S. Fix ca ~ Pic (S), c 2 ~ H4(S, ~E) ~ ~E, r 6 Z, r > 1. Let MH(r, c a, c2) be the moduli scheme of H-stable vector bundles of rank r with first Chern class c a and second Chern class c 2 (see [16]). If S = ~2, G. Ellingsrud in [8] proved that Mn (r, ca, c2) is irreducible (if not empty). His construction proved also that Mn (r, Cl, c2) is unirational and for some choice of r, c 1, c 2 even stably rational ([1]). The proofs in [8] are based on [6]. The same methods apply for many other surfaces, in particular for the minimal rational surfaces (see Proposition 2.1). The aim of this paper is to show that this happens (at least for suitable H) for every rational surface. It is natural to ask if this is true for all ample line bundles. For the existence of simple vector bundles on certain rational surfaces, see [2], [19]. In the first version of this paper the main result was stated only for r = 2. The referee remarked that the same proof works in general.

15 citations



Journal ArticleDOI
Gerd Rudolph1
TL;DR: In this article, the problem of lifting the action of a symmetry group K on spacetime M to automorphisms of a principal bundle P(M, G) is discussed and a classification of bundles P admitting a lift is given for a case more general than that considered by Harnad, Shnider, and Vinet.
Abstract: The problem of lifting the action of a symmetry group K on spacetime M to automorphisms of a principal bundle P(M, G) is discussed. A classification of bundles P admitting a lift is given for a case more general than that considered by Harnad, Shnider, and Vinet.

Journal ArticleDOI
TL;DR: In this paper, the tangent bundle of a closed, connected, non-orientable smooth manifold is embedded as a sub-bundle of a 2-plane bundle over a CW complex of dimension m or less.
Abstract: Let ζ be a nonorientable m-plane bundle over a CW complex X of dimension m or less Given a 2-plane bundle η over X, we wish to know whether η can be embedded as a sub-bundle of ζ The bundle η need not be orientable When ζ is even-dimensional there is the added complication of twisted coefficients In that case, we use Postnikov decomposition of certain nonsimple fibrations in order to describe the obstructions for the embedding problem Emery Thomas [11] and [12] treated this problem for ζ and η both orientable The results found here are applied to the tangent bundle of a closed, connected, nonorientable smooth manifold, as a special case


Journal ArticleDOI
Simon Davis1
TL;DR: The connection form of a fiber bundle may be identified with the gauge potential of a Yang-Mills theory only if its dependence on the coordinates of the fibres can be eliminated as mentioned in this paper.


Journal Article
TL;DR: The only known holomorphic rank 2 vector bündle on P for n > 4 is the Horrocks-Mumford bundle as discussed by the authors, which has Chern-classes ci(d) = −d and c2(d), where d is the degree of the morphism.
Abstract: The only known holomorphic rank 2 vector bündle on P\" for n > 4 (except direct sums of line bundles) is the Horrocks-Mumford bündle ^ on P, [H-M], 1973. Of course this is not quite true, since we may twist &* by a line bündle or may pull ̂ back under a finite morphism n: P — > /P. 2F is stable and has Chern-classes ci = — l and c2 = 4 (for a suitable twist). *^ is stable too, cf. [Ba], and has Chern-classes ci(d) = —d and c2(d) = 4d where d is the degree of . Let M(d) = {n: P— > P> of degree d} denote the variety of finite morphisms. Pulling back induces a morphism



Journal ArticleDOI
TL;DR: In this paper, a new interpretation of a particular fiber-bundle structure constructed on the timelike homogeneous space M=SO(4,2)/SO (4,1) is presented, and Minkowski space-time is realized as a subspace of the standard fiber of the tangent bundle over this hyperquadric.
Abstract: A hyper‐relativistic system is defined as one whose equation of motion is form invariant under coordinate transformations induced by a semisimple group whose algebra is contractible to the algebra of the Poincare group. Such a system lies, categorically, in the domain between the special theory of relativity and the general theory, for whereas the former requires covariance under transformations between inertial systems, the latter imposes covariance with respect to arbitrary continuous transformations. In this paper, a new interpretation of a particular fiber‐bundle structure constructed on the timelike homogeneous space M=SO(4,2)/SO(4,1) is presented, and Minkowski space‐time is realized as a subspace of the standard fiber of the tangent bundle over this hyperquadric. Through the process of group contraction, coupled with the commutation of the momentum vector fields with the principal bundle of linear frames with which the tangent bundle is associated, a hierarchy of ‘‘Heisenberg commutation relations,...