# Lie bracket of vector fields

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In the mathematical field of differential topology, the Lie bracket of vector fields, also known as the JacobiLie bracket or the commutator of vector fields, is an operator that assigns to any two vector fields X and Y on a smooth manifold M a third vector field denoted [X, Y].

## Contents

Conceptually, the Lie bracket [X, Y] is the derivative of Y along the flow generated by X, and is sometimes denoted ${\displaystyle {\mathcal {L}}_{X}Y}$ ("Lie derivative of Y along X"). This generalizes to the Lie derivative of any tensor field along the flow generated by X.

The Lie bracket is an R-bilinear operation and turns the set of all smooth vector fields on the manifold M into an (infinite-dimensional) Lie algebra.

The Lie bracket plays an important role in differential geometry and differential topology, for instance in the Frobenius integrability theorem, and is also fundamental in the geometric theory of nonlinear control systems. [1]

## Definitions

There are three conceptually different but equivalent approaches to defining the Lie bracket:

### Vector fields as derivations

Each smooth vector field ${\displaystyle X:M\rightarrow TM}$ on a manifold M may be regarded as a differential operator acting on smooth functions ${\displaystyle f(p)}$ (where ${\displaystyle p\in M}$ and ${\displaystyle f}$ of class ${\displaystyle C^{\infty }(M)}$) when we define ${\displaystyle X(f)}$ to be another function whose value at a point ${\displaystyle p}$ is the directional derivative of f at p in the direction X(p). In this way, each smooth vector field X becomes a derivation on C(M). Furthermore, any derivation on C(M) arises from a unique smooth vector field X.

In general, the commutator ${\displaystyle \delta _{1}\circ \delta _{2}-\delta _{2}\circ \delta _{1}}$ of any two derivations ${\displaystyle \delta _{1}}$ and ${\displaystyle \delta _{2}}$ is again a derivation, where ${\displaystyle \circ }$ denotes composition of operators. This can be used to define the Lie bracket as the vector field corresponding to the commutator derivation:

${\displaystyle [X,Y](f)=X(Y(f))-Y(X(f))\;\;{\text{ for all }}f\in C^{\infty }(M).}$

### Flows and limits

Let ${\displaystyle \Phi _{t}^{X}}$ be the flow associated with the vector field X, and let D denote the tangent map derivative operator. Then the Lie bracket of X and Y at the point xM can be defined as the Lie derivative:

${\displaystyle [X,Y]_{x}\ =\ ({\mathcal {L}}_{X}Y)_{x}\$ :=\ \lim _{t\to 0}{\frac {(\mathrm {D} \Phi _{-t}^{X})Y_{\Phi _{t}^{X}(x)}\,-\,Y_{x}}{t}}\ =\ \left.{\tfrac {\mathrm {d} }{\mathrm {d} t}}\right|_{t=0}(\mathrm {D} \Phi _{-t}^{X})Y_{\Phi _{t}^{X}(x)}.}

This also measures the failure of the flow in the successive directions ${\displaystyle X,Y,-X,-Y}$ to return to the point x:

${\displaystyle [X,Y]_{x}\ =\ \left.{\tfrac {1}{2}}{\tfrac {\mathrm {d} ^{2}}{\mathrm {d} t^{2}}}\right|_{t=0}(\Phi _{-t}^{Y}\circ \Phi _{-t}^{X}\circ \Phi _{t}^{Y}\circ \Phi _{t}^{X})(x)\ =\ \left.{\tfrac {\mathrm {d} }{\mathrm {d} t}}\right|_{t=0}(\Phi _{\!-{\sqrt {t}}}^{Y}\circ \Phi _{\!-{\sqrt {t}}}^{X}\circ \Phi _{\!{\sqrt {t}}}^{Y}\circ \Phi _{\!{\sqrt {t}}}^{X})(x).}$

### In coordinates

Though the above definitions of Lie bracket are intrinsic (independent of the choice of coordinates on the manifold M), in practice one often wants to compute the bracket in terms of a specific coordinate system ${\displaystyle \{x^{i}\}}$. We write ${\displaystyle \partial _{i}={\tfrac {\partial }{\partial x^{i}}}}$ for the associated local basis of the tangent bundle, so that general vector fields can be written ${\displaystyle \textstyle X=\sum _{i=1}^{n}X^{i}\partial _{i}}$and ${\displaystyle \textstyle Y=\sum _{i=1}^{n}Y^{i}\partial _{i}}$for smooth functions ${\displaystyle X^{i},Y^{i}:M\to \mathbb {R} }$. Then the Lie bracket can be computed as:

${\displaystyle [X,Y]:=\sum _{i=1}^{n}\left(X(Y^{i})-Y(X^{i})\right)\partial _{i}=\sum _{i=1}^{n}\sum _{j=1}^{n}\left(X^{j}\partial _{j}Y^{i}-Y^{j}\partial _{j}X^{i}\right)\partial _{i}.}$

If M is (an open subset of) Rn, then the vector fields X and Y can be written as smooth maps of the form ${\displaystyle X:M\to \mathbb {R} ^{n}}$ and ${\displaystyle Y:M\to \mathbb {R} ^{n}}$, and the Lie bracket ${\displaystyle [X,Y]:M\to \mathbb {R} ^{n}}$ is given by:

${\displaystyle [X,Y]:=J_{Y}X-J_{X}Y}$

where ${\displaystyle J_{Y}}$ and ${\displaystyle J_{X}}$ are n × n Jacobian matrices (${\displaystyle \partial _{j}Y^{i}}$ and ${\displaystyle \partial _{j}X^{i}}$ respectively using index notation) multiplying the n × 1 column vectors X and Y.

## Properties

The Lie bracket of vector fields equips the real vector space ${\displaystyle V=\Gamma (TM)}$ of all vector fields on M (i.e., smooth sections of the tangent bundle ${\displaystyle TM\to M}$) with the structure of a Lie algebra, which means [ • , • ] is a map ${\displaystyle V\times V\to V}$ with:

• R-bilinearity
• Anti-symmetry, ${\displaystyle [X,Y]=-[Y,X]}$
• Jacobi identity, ${\displaystyle [X,[Y,Z]]+[Z,[X,Y]]+[Y,[Z,X]]=0.}$

An immediate consequence of the second property is that ${\displaystyle [X,X]=0}$ for any ${\displaystyle X}$.

Furthermore, there is a "product rule" for Lie brackets. Given a smooth (scalar-valued) function f on M and a vector field Y on M, we get a new vector field fY by multiplying the vector Yx by the scalar f(x) at each point xM. Then:

• ${\displaystyle [X,fY]\ =\ X\!(f)\,Y\,+\,f\,[X,Y],}$

where we multiply the scalar function X(f) with the vector field Y, and the scalar function f with the vector field [X, Y]. This turns the vector fields with the Lie bracket into a Lie algebroid.

Vanishing of the Lie bracket of X and Y means that following the flows in these directions defines a surface embedded in M, with X and Y as coordinate vector fields:

Theorem:${\displaystyle [X,Y]=0\,}$ iff the flows of X and Y commute locally, meaning ${\displaystyle (\Phi _{t}^{Y}\Phi _{s}^{X})(x)=(\Phi _{s}^{X}\,\Phi _{t}^{Y})(x)}$ for all xM and sufficiently small s, t.

This is a special case of the Frobenius integrability theorem.

## Examples

For a Lie group G, the corresponding Lie algebra ${\displaystyle {\mathfrak {g}}}$ is the tangent space at the identity ${\displaystyle T_{e}G}$, which can be identified with the vector space of left invariant vector fields on G. The Lie bracket of two left invariant vector fields is also left invariant, which defines the Jacobi–Lie bracket operation ${\displaystyle [\,\cdot \,,\,\cdot \,]:{\mathfrak {g}}\times {\mathfrak {g}}\to {\mathfrak {g}}}$.

For a matrix Lie group, whose elements are matrices ${\displaystyle g\in G\subset M_{n\times n}(\mathbb {R} )}$, each tangent space can be represented as matrices: ${\displaystyle T_{g}G=g\cdot T_{I}G\subset M_{n\times n}(\mathbb {R} )}$, where ${\displaystyle \cdot }$ means matrix multiplication and I is the identity matrix. The invariant vector field corresponding to ${\displaystyle X\in {\mathfrak {g}}=T_{I}G}$ is given by ${\displaystyle X_{g}=g\cdot X\in T_{g}G}$, and a computation shows the Lie bracket on ${\displaystyle {\mathfrak {g}}}$ corresponds to the usual commutator of matrices:

${\displaystyle [X,Y]\ =\ X\cdot Y-Y\cdot X.}$

## Applications

The JacobiLie bracket is essential to proving small-time local controllability (STLC) for driftless affine control systems.

## Generalizations

As mentioned above, the Lie derivative can be seen as a generalization of the Lie bracket. Another generalization of the Lie bracket (to vector-valued differential forms) is the Frölicher–Nijenhuis bracket.

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## References

• "Lie bracket", Encyclopedia of Mathematics , EMS Press, 2001 [1994]
• Isaiah, Pantelis (2009), "Controlled parking [Ask the experts]", IEEE Control Systems Magazine, 29 (3): 17–21, 132, doi:10.1109/MCS.2009.932394, S2CID   42908664
• Khalil, H.K. (2002), Nonlinear Systems (3rd ed.), Upper Saddle River, NJ: Prentice Hall, ISBN   0-13-067389-7
• Kolář, I., Michor, P., and Slovák, J. (1993), Natural operations in differential geometry, Springer-VerlagCS1 maint: multiple names: authors list (link) Extensive discussion of Lie brackets, and the general theory of Lie derivatives.
• Lang, S. (1995), Differential and Riemannian manifolds, Springer-Verlag, ISBN   978-0-387-94338-1 For generalizations to infinite dimensions.
• Lewis, Andrew D., Notes on (Nonlinear) Control Theory (PDF)
• Warner, Frank (1983) [1971], Foundations of differentiable manifolds and Lie groups, New York-Berlin: Springer-Verlag, ISBN   0-387-90894-3