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The Stacks project

Remark 42.56.2. Let X be a scheme such that 2 is invertible on X. Then the Adams operator \psi ^2 can be defined on the K-group K_0(X) = K_0(D_{perf}(\mathcal{O}_ X)) (Derived Categories of Schemes, Definition 36.38.2) in a straightforward manner. Namely, given a perfect complex L on X we get an action of the group \{ \pm 1\} on L \otimes ^\mathbf {L} L by switching the factors. Then we can set

\psi ^2(L) = [(L \otimes ^\mathbf {L} L)^+] - [(L \otimes ^\mathbf {L} L)^-]

where (-)^+ denotes taking invariants and (-)^- denotes taking anti-invariants (suitably defined). Using exactness of taking invariants and anti-invariants one can argue similarly to the proof of Lemma 42.56.1 to show that this is well defined. When 2 is not invertible on X the situation is a good deal more complicated and another approach has to be used.


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