Differential pullback along a diffeomorphism
Let
The pushforward can be defined via the inverse so that
Further terminology
- If
and𝜑 ∈ A u t 𝖬 𝖺 𝗇 𝛼 ( 𝑀 ) , we say𝜑 ∗ 𝑇 = 𝑇 is a symmetry transformation of the tensor field𝜑 .𝑇 - In the particular case
for the metric tensor, we say𝜑 ∗ 𝑔 = 𝑔 is an isometry of𝜑 .𝑀
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