Differential geometry MOC

Differential pushforward

Let πœ‘ :𝑀 →𝑁 be a 𝐢𝛼-map. The pushforward πœ‘βˆ— is an operation for β€œpushing forward” data defined on 𝑀 to data defined on 𝑁. Usually this corresponds to some kind of postcomposition in the sense of Pushforward and pullback of morphisms.

Differential pushforward of a vector field

Let 𝑣 βˆˆπ”›(𝑀) be a vector field on 𝑀. As a derivation on 𝐢𝛼(𝑁), the pushforward πœ‘βˆ—π‘£ βˆˆπ”›(𝑁) is defined by #m/def/geo/diff

(πœ‘βˆ—π‘£)(𝑓)=𝑣(πœ‘βˆ—π‘“)

where πœ‘βˆ—π‘“ =𝑓 βˆ˜πœ‘ is the Differential pullback of a scalar field 𝑓 βˆˆπΆπ›Ό(𝑀). This is equivalent to the Tangent map acting on the tangent space or bundle of 𝑀.

Differential pushforward of a contravariant tensor field

The above may be viewed as a special case of the following. Let 𝑇 ∈T𝑝0(𝑀) be a totally contravariant tensor field. The pushforward πœ‘βˆ—π‘‡ ∈T𝑝0(𝑁) is defined by #m/def/geo/diff

(πœ‘βˆ—π‘‡)π‘Ž1β‹―π‘Žπ‘(πœ”1)π‘Ž1β‹―(πœ”π‘)π‘Žπ‘:=π‘‡π‘Ž1β‹―π‘Žπ‘(πœ‘βˆ—πœ”1)π‘Ž1β‹―(πœ‘βˆ—πœ”π‘)π‘Žπ‘

for 1-forms (πœ”1)π‘Ž,…,(πœ”π‘)π‘Ž ∈Ω1(𝑀), where πœ‘βˆ— denotes the differential pullback of a 1-form.

For mixed tensor fields it is in general not possible to define the pushforward, except for the special case of the Differential pullback along a diffeomorphism.


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