Differential geometry MOC

Differential pullback along a diffeomorphism

Let πœ‘ :𝑀 →𝑁 be a 𝐢𝛼-diffeomorphism. For a mixed tensor field π‘‡π‘Ž1β‹―π‘Žπ‘π‘1β‹―π‘π‘ž ∈Tπ‘π‘ž(𝑁), the pullback πœ‘βˆ—π‘‡π‘Ž1β‹―π‘Žπ‘π‘1β‹―π‘π‘ž ∈Tπ‘π‘ž(𝑀) is defined by diff

(πœ‘βˆ—π‘‡)π‘Ž1β‹―π‘Žπ‘π‘1β‹―π‘π‘ž(πœ”1)π‘Ž1β‹―(πœ”π‘)π‘Žπ‘(𝑣1)𝑏1β‹―(π‘£π‘ž)π‘π‘ž=π‘‡π‘Ž1β‹―π‘Žπ‘π‘1β‹―π‘π‘ž(πœ‘βˆ—πœ”1)π‘Ž1β‹―((πœ‘βˆ’1)βˆ—π‘£π‘ž)π‘π‘ž.

The pushforward can be defined via the inverse so that

(πœ‘βˆ’1)βˆ—=πœ‘βˆ—:Tπ‘π‘ž(𝑁)β†’Tπ‘π‘ž(𝑀).

Further terminology

  • If πœ‘ ∈Aut𝖬𝖺𝗇𝛼⁑(𝑀) and πœ‘βˆ—π‘‡ =𝑇, we say πœ‘ is a symmetry transformation of the tensor field 𝑇.
  • In the particular case πœ‘βˆ—π‘” =𝑔 for the metric tensor, we say πœ‘ is an isometry of 𝑀.


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