nLab Lie bracket of vector fields

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Contents

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 infinitesimal infinitesimal & 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

Definition

Given a smooth manifold XX, the Lie bracket of vector fields uu and vv can be defined in several ways.

As commutator of derivations

Since derivations of smooth functions are vector fields, we can identify uu and vv with the corresponding derivations C (X)C (X)C^\infty(X)\to C^\infty(X).

Taking the commutator uvvuu v-v u of these derivations produces another derivation, which is denoted by [u,v][u,v], and which can be identified with a vector field on XX.

As a Lie derivative

Alternatively, we can set

[u,v]= uv= vu,[u,v]=\mathcal{L}_u v=-\mathcal{L}_v u,

where \mathcal{L} denotes the Lie derivative of a vector field.

Properties

The real vector space of vector fields on XX equipped with the Lie bracket forms a Lie algebra.

Last revised on May 3, 2023 at 09:44:05. See the history of this page for a list of all contributions to it.