Created: 2026-03-06 07:59:30
Updated: 2026-03-06 08:17:22

9.1 Tangent Bundles

A tangent bundle TMTM over an mm-dimensional manifold MM is a collection of all tangent spaces of MM:

TMpMTpM\begin{equation} TM\equiv \bigcup_{p\in M} T_{p}M \end{equation}

The manifold MM over which TMTM is defined is called base space.

Let {Ui}\{U_{i}\} be an open covering of MM, and xμ=φi(p)x^{\mu}=\varphi_{i}(p) is the coordinate on UiU_{i}, an element of TUipUiTpMTU_{i}\equiv \bigcup_{p\in U_{i}} T_{p}M is specified by a point pMp\in M and a vector VTpMV\in T_{p}M. We find that TUiTU_{i} is identified with Rm×Rm\mathbb{R}^{m}\times \mathbb{R}^{m}. If (p,V)TUi(p,V)\in T U_{i}, the identification is given by (p,V)(xμ(p),Vμ(p))(p,V)\mapsto (x^{\mu}(p),V^{\mu}(p)), TUiTU_{i} is a 2m2m-dim differentiable manifold. We can define a natural projection π:TUiUi\pi:TU_{i}\to U_{i}, π(p,V)=p\pi(p,V)=p, and π1(p)=TpM\pi ^{-1}(p)=T_{p}M. In the context of fibre bundle theory, TpMT_{p}M is called a fibre at pp.

If M=RmM=\mathbb{R}^{m} then TM=Rm×RmTM=\mathbb{R}^{m}\times \mathbb{R}^{m}, but it is not the case for general MM, and TMTM measures topological nontriviality of MM. To see this we need to look at different charts Ui,UjU_{i},U_{j}, with UiUjU_{i}\cap U_{j}\neq \emptyset, let xμ,yμx^{\mu},y^{\mu} be their coordinates respectively. For VTpM,pUiUjV\in T_{p}M,p\in U_{i}\cap U_{j},

V=Vμxμp=V~μyμp\begin{equation} V= V^{\mu} \frac{ \partial }{ \partial x^{\mu} }|_{p} = \tilde{V}^{\mu} \frac{ \partial }{ \partial y^{\mu} }|_{p} \end{equation}

and V~μ=yνxμ(p)VμGμνVμ\tilde{V}^{\mu}=\frac{ \partial y^{\nu} }{ \partial x ^{\mu}}(p)V^{\mu}\equiv G^{\nu}_{\mu}V^{\mu}. GGL(m,R)G\in GL(m,\mathbb{R}) must be non-singular. The fibre coordinates are rotated whenever we switch to another coordinates. GL(m,R)GL(m,\mathbb{R}) is the structure group of TMTM.

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