Generalized cohomological index theories for Lie group actions with an application to bifurcation questions for Hamiltonian systems
Generalized cohomological index theories for Lie group actions with an application to bifurcation questions for Hamiltonian systems
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DOI:
10.1007/bf01390270
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发表时间:
1977
影响因子:
3.1
通讯作者:
E. Fadell;P. Rabinowitz
中科院分区:
文献类型:
--
作者:
E. Fadell;P. Rabinowitz
In another work [1] the authors employed a cohomological index (see also Yang [2, 3], Conner-Floyd [4] and Holm-Spanier [5]) in place of the usual notion of genus [6, 7] which is useful in symmetric situations with the group of symmetry being 7/2, eg, in the consideration of (odd) maps f such that f (-x)=-f (x). Replacing genus by this cohomological index was dictated by the need of additional property-the piercing property (Proposition (3.9)). In this paper we extend this idea of cohomological index to the general situation where the symmetry group is an arbitrary compact Lie group G. It turns out that any cohomology class c~ H*(Bo), where B e is the universal classifying space for G, gives rise to an integer, index, X, where X is an arbitrary paracompact free G-space, and this index enjoys (w 3), quite generally, the usual notions required of such a theory, including the piercing property. Section 4 is devoted to three important special cases, namely when c~ is specialized to the generator of the cohomology ofiFP, infinite projective space, where IF is either the reals F,,, the complex numbers~, or the quaternions IH, and the group G is the unit sphere in IF. We use the notation index~ X, index e X, index~ X, for these three cases. The first, index~ X, is equivalent in a restricted category, to the cohomological index of Yang E2, 3]. This is the index employed in [1] and it is designated in Conner-Floyd 1-4] by co-indexz2 X. In Section 5 we reformulate the theory in the setting of a normed linear space~ over IF using the notion Index r X= index r X+ 1. In applications of interest, where the underlying group of symmetry is S 1, the resulting action may not be free due to the presence of isotropy subgroups of arbitrary order. Accordingly, in Section 6, we employ the index theory developed for free G-spaces, to define index theories in the general situation, namely the category of paracompact G-spaces without the assumption of a free action. The* This research was sponsored in part by the Office of Naval Research under Contract No. N00014-76-C-0300, by the US Army under Contract No. DAAG2-75-C-0024, and in part by the National Science Foundation under Grant No. NSF MCS76-06373. Any reproduction in part or in full for the purposes of the US Government is permitted