The Heat Kernel on a Principal Bundle
We now use that the operator Q = D2 acts on sections of the vector bundle E ⊗ L, where E is the bundle (5.7), associated to the principal SpinC (2n)bundle Spinc F M. The covariant differentiation of sections of this bundle is defined by (3.45).
KeywordsVector Field Vector Bundle Laplace Operator Heat Kernel Principal Bundle
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