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Obstruction Class for the Existence of a Conformal Spin Structure in a Strict Sense
Advances in Applied Clifford Algebras ( IF 1.1 ) Pub Date : 2020-02-08 , DOI: 10.1007/s00006-020-1044-2
Pierre Anglès

Let V be a pseudo-Riemannian n-dimensional manifold or, more generally, let \((\xi ,Q)\) be a real fibre bundle whose base space is a paracompact space endowed with a non-degenerate quadratic form Q, (that is, with a structure group \({\mathrm {O}}(p,q),\)\(n=p+q\).) Let \(K_{p,q}\) denote the obstruction class for the existence of a \(\mathrm {Pin}(p,q)\)-spin structure on V or over \(\xi .\) Let \(K_{\mathrm {Conf}}(p,q)\) denote the obstruction class for the existence of a conformal spin structure in a strict sense on V or over \(\xi ,\) (simply: a \(C_{n}^{s}(p,q)\)-spin structure), if \(n=2r,\) or of a conformal special spin structure, if \(n=2r+1.\) This short self-contained paper will recall the determination of the obstruction class \(K_{p,q}\) on V, or over \(\xi ,\) for n even or odd. Then, the obstruction class \(K_{p+1,q+1}\) for the existence of a \(\mathrm {Pin}(p+1,q+1)\)-spin structure over \(\xi _{j}\), (Greub’s j-extension of \(\xi ,\) where j denotes the identity mapping from \({\mathrm {O}}(p,q)\) into \({\mathrm {O}}(p+1,q+1)\)), will be determined in order to express \(K_{\mathrm {Conf}}(p,q),\) for \(n=2r\) or \(n=2r+1,\) in terms of the Stiefel–Whitney classes \(w_{i}(p,q),\)\(i=1,2,\) of \(\xi \), decomposed as the Whitney sum \(\xi =\xi ^{+}\oplus \xi ^{-},\) where the restriction of Q to \(\xi ^{+}\) is positive definite and the restriction of Q to \(\xi ^{-}\) is negative. If \(n=2r,\) we find again results obtained in previous publications [4, 5, 7], by different methods.

中文翻译:

严格意义上共形自旋结构存在的障碍类别

V为伪黎曼n维流形,或更一般而言,令\ {{\ xi,Q} \}为实纤维束,其基空间是具有非简并二次形式Q的拟紧空间,(也就是说,具有结构组\({\ mathrm {O}}(p,q),\)\(n = p + q \)。)让\(K_ {p,q} \)表示障碍物类别在V上或在\(\ xi。\)上存在\(\ mathrm {Pin}(p,q)\)- spin结构的情况下,让\(K _ {\ mathrm {Conf}}(p,q)\ )表示在V或以上严格意义上存在共形自旋结构的障碍类别\(\ xi,\)(简单地:\(C_ {n} ^ {s}(p,q)\)- spin结构),如果\(n = 2r,\)或共形特殊自旋结构,如果\(n = 2r + 1。\)这个简短的独立论文将回顾在V上或在\(\ xi,\)上n个偶数的障碍物类\(K_ {p,q} \)的确定。或奇怪。然后,在\(\ xi上存在\(\ mathrm {Pin}(p + 1,q + 1)\)- spin结构的障碍类\(K_ {p + 1,q + 1} \)_ {Ĵ} \) ,(Greub的Ĵ的-extension \(\ XI,\)其中Ĵ表示从身份映射\({\ mathrm {O}}(p,q)\)变成\({\ mathrm {O}}(p + 1,q + 1)\)),将被确定以表达\(K_ { \ mathrm {CONF}}(p,q),\)\(N = 2R \)\(N = 2R + 1,\)在施蒂费尔-惠特尼类的术语\(W_ {I}(p, q),\)\(I = 1,2,\)\(\ XI \) ,分解为惠特尼总和\(\ XI = \ XI ^ {+} \ oplus \ XI ^ { - },\)其中Q\(\ xi ^ {+} \)的限制为正定,而Q\(\ xi ^ {-} \)的限制为负。如果\(n = 2r,\) 我们再次发现以前的出版物[4、5、7]通过不同方法获得的结果。
更新日期:2020-02-08
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