Timeline for Chern classes of generators of $K(S^{2n})$
Current License: CC BY-SA 4.0
9 events
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Jun 7, 2018 at 18:11 | comment | added | Michael Albanese | There is an error in the proof of Theorem IV 1.4, it should be $\operatorname{ch}_2E$ not $\operatorname{ch}E$. Making this adjustment, the conclusion is $\operatorname{ind}(D^+) = \frac{2^n}{(n-1)!}c_n(E)$ which is not strong enough to prove the theorem. However, using the Dirac operator coupled to $E$ gives the stated index and the correct conclusion. | |
Jun 6, 2018 at 14:09 | comment | added | Oliver Nash | Many apologies if, as it seems, I am spreading misinformation. Glancing quickly at L&M, I can't quite line up what you're saying though. Furthermore, is not Theorem IV 1.4 support for my remark? [I'll check carefully later --- for now I have to get back to the day job!] | |
Jun 6, 2018 at 13:59 | comment | added | Michael Albanese | @OliverNash: I believe that index of the signature operator coupled to $E$ is $2^n$ times the integer you mention, see Theorem III.13.9 of Lawson and Michelsohn's Spin Geometry. On the other hand, the index of the Dirac operator coupled to $E$ has this integer as its index, see Theorem III.13.10. | |
Jun 6, 2018 at 13:14 | comment | added | Oliver Nash | So, because the image of the Chern character is the integral cohomology, $c_n(E)/(n-1)!$ is an integer for any $E$. This raises the question: what is this integer that is intrinsically associated to the vector bundle E? In fact there is an answer: it is the index of the signature operator coupled to E. | |
Jun 6, 2018 at 13:13 | history | edited | Michael Albanese | CC BY-SA 4.0 |
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Jun 6, 2018 at 12:36 | history | edited | Michael Albanese | CC BY-SA 4.0 |
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Jun 6, 2018 at 2:42 | history | edited | Michael Albanese | CC BY-SA 4.0 |
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Jun 6, 2018 at 2:35 | history | edited | Michael Albanese | CC BY-SA 4.0 |
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Jun 6, 2018 at 2:27 | history | answered | Michael Albanese | CC BY-SA 4.0 |