nLab pushforward of vector fields

Redirected from "pushforward of a vector field".

Context

Differential geometry

synthetic differential geometry

Introductions

from point-set topology to differentiable manifolds

geometry of physics: coordinate systems, smooth spaces, manifolds, smooth homotopy types, supergeometry

Differentials

V-manifolds

smooth space

Tangency

The magic algebraic facts

Theorems

Axiomatics

cohesion

infinitesimal cohesion

tangent cohesion

differential cohesion

graded differential cohesion

singular cohesion

id ⊣ id ∨ ∨ fermionic ⇉ ⊣ ⇝ bosonic ⊥ ⊥ bosonic ⇝ ⊣ Rh rheonomic ∨ ∨ reduced ℜ ⊣ ℑ infinitesimal ⊥ ⊥ infinitesimal ℑ ⊣ & étale ∨ ∨ cohesive ʃ ⊣ ♭ discrete ⊥ ⊥ discrete ♭ ⊣ ♯ continuous ∨ ∨ ∅ ⊣ * \array{ && id &\dashv& id \\ && \vee && \vee \\ &\stackrel{fermionic}{}& \rightrightarrows &\dashv& \rightsquigarrow & \stackrel{bosonic}{} \\ && \bot && \bot \\ &\stackrel{bosonic}{} & \rightsquigarrow &\dashv& \mathrm{R}\!\!\mathrm{h} & \stackrel{rheonomic}{} \\ && \vee && \vee \\ &\stackrel{reduced}{} & \Re &\dashv& \Im & \stackrel{infinitesimal}{} \\ && \bot && \bot \\ &\stackrel{infinitesimal}{}& \Im &\dashv& \& & \stackrel{\text{étale}}{} \\ && \vee && \vee \\ &\stackrel{cohesive}{}& \esh &\dashv& \flat & \stackrel{discrete}{} \\ && \bot && \bot \\ &\stackrel{discrete}{}& \flat &\dashv& \sharp & \stackrel{continuous}{} \\ && \vee && \vee \\ && \emptyset &\dashv& \ast }

Models

Lie theory, ∞-Lie theory

differential equations, variational calculus

Chern-Weil theory, ∞-Chern-Weil theory

Cartan geometry (super, higher)

Contents

Idea

Given a differentiable map ϕ:X 1→X 2\phi \colon X_1 \xrightarrow{\;} X_2 between differentiable manifolds (e.g. a smooth map between smooth manifolds) and thinking of vector fields as infinitesimal approximations to differentiable curves

T xX≃{γ∈C ∞(ℝ,X)|γ(0)=x}/(γ 1∼γ 2⇔dγ 1(0)=dγ 2(0)) T_x X \;\simeq\; \big\{ \gamma \in C^\infty\big(\mathbb{R},\, X\big) \,\big\vert\, \gamma(0) = x \big\} \Big/ \big( \gamma_1 \sim \gamma_2 \;\Leftrightarrow\; \mathrm{d}\gamma_1(0) = \mathrm{d}\gamma_2(0) \big)

then the postcomposition of these curves with ϕ\phi induces maps of equivalence classes

T xX 1 →−− T ϕ(x)X 2 [γ] ↦ [ϕ∘γ] \begin{array}{ccc} T_x X_1 &\xrightarrow{\phantom{--}}& T_{\phi(x)} X_2 \\ [\gamma] &\mapsto& [\phi \circ \gamma] \end{array}

alternatively denoted “ϕ *\phi_\ast” or “dϕ\mathrm{d}\phi” (cf. differentiation as a functor) and called the pushforward of vector fields along ϕ\phi.

Literature

Most texts on differential geometry will discuss pushforward of vector fields.

See also

Created on June 21, 2024 at 09:45:41. See the history of this page for a list of all contributions to it.