PlanetMath: jet bundle

(more info)

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jet bundle

(Definition)

Introduction

Let $p\colon X\to B$ be a surjective submersion of $\mathcal{C}^r$ differential manifolds, where $r\in\{0,1,\ldots\}\cup\{\infty,\omega\}$ ( $\mathcal{C}^\omega$ means real analytic). For all integers $k\ge 0$ with $k\le r$ , we will define a fibre bundle $\mathrm{J}^k_B X$ over

, called the

-th jet bundle of

over

. The fibre of this bundle above a point $x\in X$ can be interpreted as the set of equivalence classes of local sections of

passing through

, where two sections are considered equivalent if their first

derivatives at

are equal. The equivalence class of a section is then the jet of that section; it indicates the direction of the section locally at

. This concept has much in common with that of the germ of a smooth function on a manifold: it contains not only the value of a function at a point, but also some information about the behaviour of the function near that point.

Construction

We will now define each jet bundle of

over

as a set with a projection map to

, and we describe the concept of prolongation of sections. After that, we give a slightly different construction allowing us to put a manifold structure on each of the jet bundles.

For every open subset of , we denote by $\Gamma(U,X)$ the set of sections of over , i.e. the set of ${\cal C}^r$ functions $s\colon U\to p^{-1}U$ such that $p\vert_{p^{-1}U}\circ s=\mathop{\rm id}_U$ . Every point of has an open subset such that there exists at least one section of over , due to the assumption that is a surjective submersion. For all $x\in X$ , we define the fibre of $\mathrm{J}^k_BX$ above by

$\displaystyle \mathrm{J}^k_BX(x)=\{(U,s)\colon U\subset B\hbox{ open}, x\in U,s\in\Gamma(U,X),s(p(x))=x\}/\mathord\sim,$

where the equivalence relation $\sim$ is defined by $s\sim s'\Leftrightarrow s$ and

induce the same map between the fibres at

and

of the

-th iterated tangent bundles of

and

, respectively. (Note that the fibres in the

-th iteration are the same if and only if the induced maps are already the same in the

-st iteration). We will denote the equivalence class of a pair

. As a set, $\mathrm{J}^k_BX$ is defined as the disjoint union of the sets $\mathrm{J}^k_BX(x)$ with $x\in X$ . Write $\pi\colon \mathrm{J}^k_BX\to X$ for the `obvious' projection map, defined by

$\displaystyle \pi([U,s])=x\hbox{ for }[U,s]\in\mathrm{J}^k_BX(x).$

Notice that $\mathrm{J}^0_BX$ is just

itself.

Suppose we have some section of over an open subset of . By sending every point $y\in U$ to the equivalence class $[U,s]\in\mathrm{J}^k_BX(s(y))$ we obtain a section of $\pi\circ p\colon \mathrm{J}^k_BX\to B$ over for each $k\ge 0$ , called the -th prolongation of . Composing this section on the left with $\pi$ gives back the original section of .

The bundle structure

Instead of defining all the jet bundles at once, we may choose to define only the first jet bundle in the way described above. After equipping the first jet bundle with the structure of a differential manifold, which we will do below, we can then inductively define $\mathrm{J}^{k+1}_BX$ as the first jet bundle of $\mathrm{J}^k_BX$ over

for $k\ge 1$ . This is useful because the manifold structure only needs to be defined for $\mathrm{J}^1_BX$ .

We make $\mathrm{J}^1_BX$ into an affine bundle over , locally trivial of rank $\dim B(\dim X-\dim B)$ , in the following way. We cover with charts $(W,\phi,W')$ , where $\phi$ is a diffeomorphism between open subsets $W\subset X$ and $W'\subset\mathbb{R}^n$ . Without loss of generality, we assume that is contained in the domain of a chart $(V,\psi,V')$ on , with $V'\subset\mathbb{R}^m$ . Here and are the local dimensions of and , respectively.

For all $x\in W$ and all $[U,s]\in\mathrm{J}^1_BX(x)$ , we have the tangent map $\mathrm{T}s(p(x))$ , which is a linear map from $\mathrm{T}V(p(x))$ to $\mathrm{T}W(x)$ . These tangent spaces are isomorphic to $\mathbb{R}^m$ and $\mathbb{R}^n$ via the chosen charts, so that $\mathrm{T}s(p(x))$ acts as a matrix $M_x([U,s])\in\mathbb{R}^{n\times m}$ :

$\displaystyle \begin{xy} *!C\xybox{ \xymatrix{ \mathrm{T}W(x) \ar[r]^\simeq & \... ...mathrm{T}s(p(x))} \ar[r]^\simeq & \mathbb{R}^m \ar[u]_{M_x([U,s])} } } \end{xy}$

The definition of the equivalence relation $\sim$ on $\mathrm{J}^1_BX(x)$ means that the association $[U,s]\mapsto M_x([U,s])$ is well-defined and injective for each $x\in W$ . The image of

consists of the matrices with the property that multiplying them on the left with the $m\times n$ matrix corresponding to the tangent map $\mathrm{T}p(x)$ gives the $m\times m$ identity matrix. These matrices form a

-dimensional linear subspace $L_x\subset\mathbb{R}^{n\times m}$ , and $L=\bigcup_{x\in W}\{x\}\times L_x$ is a submanifold of $W\times\mathbb{R}^{n\times m}$ .

We fix both the differentiable structure of $\pi^{-1}U$ and a local trivialisation of $\mathrm{J}^1_BX$ as a vector bundle by requiring that

$\displaystyle \pi^{-1}W$	$\displaystyle \to$	$\displaystyle L$
$\displaystyle {}[U,s]$	$\displaystyle \mapsto$	$\displaystyle \left(\pi([U,s]),M_{\pi([U,s])}([U,s])\right)$

be a diffeomorphism and an $\mathbb{R}$ -linear map. Since the effect of a change of charts on

is multiplying each

by matrices depending differentiably on $x\in W$ (namely, the derivatives of the glueing maps), this gives a well-defined vector bundle structure on all of $\mathrm{J}^1_BX$ .

Iterating the above construction by defining $\mathrm{J}^{k+1}_BX$ as the first jet bundle of $\mathrm{J}^k_BX$ over , each jet bundle $\mathrm{J}^{k+1}_BX$ becomes a vector bundle over $\mathrm{J}^k_BX$ and a fibre bundle over . Normally, only $\mathrm{J}^1_BX$ is a vector bundle over .