WebKervaire and Milnor [20] showed that the answer is \Yes" unless n= 4k+2; but that there is an obstruction, the Kervaire invariant : fr 4k+2!Z=2Z; which vanishes on a cobordism class if and only if the class contains a homotopy sphere. Kervaire’s construction [19] of a PL 10-manifold with no smooth structure amounted to showing that = 0 on fr 10 WebGENERALIZATIONS OF THE KERVAIRE INVARIANT 369 LEMMA (1.2). {S2n, Kj} Z2 . Let ," {S2n, K.} be the generator. We view u E Hn(X) as a map u: X Kn. If v E H2n(X), there is a map g,: X S2n such that g*(s2,) = v, where S2n c H2n(S2n) is the generator. Define F(u, …
Generalizations of the Kervaire Invariant - JSTOR
WebSep 30, 1994 · A quick recollection of Browder's and Brown's generalizations of the Kervaire invariant, change of Wu-orientations and the preferred orientation To cut short the presentation we refer the reader to [1-5] for the necessary details of the notations we are going to use in the following discussion. Let M` be a smooth manifold (Poincarduality … WebThen the Arf invariant is a well-de ned element of k=P. In particular, if k= F 2, then the Arf-invariant is de ned in F 2. Theorem 6 (Arf). Nondegenerate quadratic forms over a eld kof characteristic 2 are completely classi ed by their dimension and their Arf invariant. 3 The Kervaire invariant 3.1 The Kervaire invariant for framed manifolds De ... how many radians are in 360 deg
The Kervaire Invariant of Framed Manifolds and its …
Webthe appearance of an analogue to the Kervaire invariant [7: ? 8]. An interesting by-product of this investigation will be the fact that these invariants seem to detect the differentiable structure on the knot in half the cases (i.e.; knots in (4q - 1)-space. See ? 3.2 and 3.3), but ignore it in the other half ((4q + 1)-space). WebWe will consider its generalization to more general spacetime dimensions and to more general spacetime structures, and show that this action is projective up to a multiplication by an invertible topological phase, whose partition … WebNov 25, 2024 · We consider an analogue of Witten’s SL(2, ℤ) action on three-dimensional QFTs with U(1) symmetry for 2k-dimensional QFTs with ℤ2 (k − 1)-form symmetry. We show that the SL(2, ℤ) action only closes up to a multiplication by an invertible topological phase whose partition function is the Brown-Kervaire invariant of the spacetime manifold. We … how deep do you have to be to survive a nuke