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In [[mathematics]], particularly [[differential topology]], the '''secondary vector bundle structure'''
refers to the natural [[vector bundle]] structure (''TE'',''p''<sub>*</sub>,''TM'') on the total space ''TE'' of the [[tangent bundle]] of a smooth vector bundle (''E'',''p'',''M''), induced by the push-forward ''p''<sub>*</sub>:''TE''&rarr;''TM'' of the original projection map ''p'':''E''&rarr;''M''.


In the special case (''E'',''p'',''M'')=(''TM'',&pi;<sub>''TM''</sub>,''M''), where ''TE''=''TTM'' is the [[double tangent bundle]], the secondary vector bundle (''TTM'',(&pi;<sub>''TM''</sub>)<sub>*</sub>,''TM'') is isomorphic to the [[tangent bundle]]
(''TTM'',&pi;<sub>''TTM''</sub>,''TM'') of ''TM'' through the [[double tangent bundle|canonical flip]].


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== Construction of the secondary vector bundle structure ==
 
Let (''E'',''p'',''M'') be a smooth vector bundle of rank ''N''. Then the preimage (''p''<sub>*</sub>)<sup>-1</sup>(X)⊂''TE'' of any tangent vector ''X''&isin;''TM'' in the push-forward ''p''<sub>*</sub>:''TE''&rarr;''TM'' of the canonical projection ''p'':''E''&rarr;''M'' is a smooth submanifold of dimension 2''N'', and it becomes a vector space with the push-forwards
:<math>
+_*:T(E\times E)\to TE \quad , \quad \lambda_*:TE\to TE
</math>
of the original addition and scalar multiplication
:<math>
+:E\times E\to E \qquad , \qquad \lambda:E\to E</math>
as its vector space operations. The triple (''TE'',''p''<sub>*</sub>,''TM'') becomes a smooth vector bundle with these vector space operations on its fibres.
 
=== Proof ===
 
Let (''U'',&phi;) be a local coordinate system on the base manifold ''M'' with &phi;(''x'')=(''x''<sup>1</sup>,...,''x''<sup>n</sup>) and let
:<math>
\psi:W \to \varphi(U)\times \mathbb R^N \quad ; \quad \psi(v^k e_k|_x) := (x^1,\ldots,x^n,v^1,\ldots,v^N)
</math>
be a coordinate system on ''E'' adapted to it. Then
:<math>
p_*\Big(X^k\frac{\partial}{\partial x^k}\Big|_v + Y^\ell\frac{\partial}{\partial v^\ell}\Big|_v\Big) = X^k\frac{\partial}{\partial x^k}\Big|_{p(v)},
</math>
so the fiber of the secondary vector bundle structure at ''X''&isin;''T''<sub>''x''</sub>''M'' is of the form
:<math>
p^{-1}_*(X) = \Big\{ \ X^k\frac{\partial}{\partial x^k}\Big|_v + Y^\ell\frac{\partial}{\partial v^\ell}\Big|_v
\ \Big| \ v\in E_x \ , \ Y^1,\ldots,Y^N\in\R \ \Big\}.
</math>
Now it turns out that
:<math>
\chi\Big(X^k\frac{\partial}{\partial x^k}\Big|_v + Y^\ell\frac{\partial}{\partial v^\ell}\Big|_v\Big) = \Big(X^k\frac{\partial}{\partial x^k}\Big|_{p(v)}, (v^1,\ldots,v^N,Y^1,\ldots,Y^N) \Big)
</math>
gives a local trivialization &chi;:''TW''&rarr;''TU''×'''R'''<sup>2''N''</sup> for (''TE'',''p''<sub>*</sub>,''TM''), and the push-forwards of the original vector space operations read in the adapted coordinates as
:<math>
\Big(X^k\frac{\partial}{\partial x^k}\Big|_v + Y^\ell\frac{\partial}{\partial v^\ell}\Big|_v\Big)
 
+_*
\Big(X^k\frac{\partial}{\partial x^k}\Big|_w + Z^\ell\frac{\partial}{\partial v^\ell}\Big|_w\Big)
 
=
X^k\frac{\partial}{\partial x^k}\Big|_{v+w} + (Y^\ell+Z^\ell)\frac{\partial}{\partial v^\ell}\Big|_{v+w}
</math>
and
:<math>
\lambda_*\Big(X^k\frac{\partial}{\partial x^k}\Big|_v + Y^\ell\frac{\partial}{\partial v^\ell}\Big|_v\Big)
 
=
X^k\frac{\partial}{\partial x^k}\Big|_{\lambda v} + \lambda Y^\ell\frac{\partial}{\partial v^\ell}\Big|_{\lambda v},
</math>
so each fibre (''p''<sub>*</sub>)<sup>-1</sup>(''X'')⊂''TE'' is a vector space and the triple (''TE'',''p''<sub>*</sub>,''TM'') is a smooth vector bundle.
 
== Linearity of connections on vector bundles ==
 
The general [[Ehresmann connection]]
:<math>
TE = HE \oplus VE
</math>
on a vector bundle (''E'',''p'',''M'') can be characterized in terms of the '''connector map'''
:<math>
\kappa:T_vE\to E_{p(v)} \qquad ; \qquad \kappa(X):=\operatorname{vl}_v^{-1}(\operatorname{vpr}X),
</math>
where vl<sub>''v''</sub>:''E''&rarr;''V''<sub>''v''</sub>''E'' is the [[vector bundle|vertical lift]],  and vpr<sub>''v''</sub>:''T''<sub>''v''</sub>''E''&rarr;''V''<sub>''v''</sub>''E'' is the [[Ehresmann connection|vertical projection]]. The mapping
:<math>
\nabla:TM\times\Gamma(E)\to\Gamma(E) \quad ; \quad \nabla_Xv := \kappa(v_*X)
</math>
induced by an Ehresmann connection is a [[covariant derivative]] on &Gamma;(''E'') in the sense that
*<math> \nabla_{X+Y}v = \nabla_X v + \nabla_Y v</math>
*<math> \nabla_{\lambda X}v=\lambda \nabla_Xv</math>
*<math> \nabla_X(v+w) = \nabla_X v + \nabla_X w</math>
*<math> \nabla_X(\lambda v)=\lambda \nabla_Xv</math>
*<math> \nabla_X(fv) = X[f]v + f\nabla_Xv</math>
if and only if the connector map is linear with respect to the secondary vector bundle structure (''TE'',''p''<sub>*</sub>,''TM'') on ''TE''. Then the connection is called ''linear''. Note that the connector map is automatically linear with respect to the tangent bundle structure (''TE'',&pi;<sub>''TE''</sub>,''E'').
 
== See also ==
* [[Connection (vector bundle)]]
* [[Double tangent bundle]]
* [[Ehresmann connection]]
* [[Vector bundle]]
 
== References ==
 
* P.Michor. ''Topics in Differential Geometry,'' American Mathematical Society (2008).
 
[[Category:Differential geometry]]
[[Category:Topology]]
[[Category:Differential topology]]

Revision as of 09:27, 23 February 2013

In mathematics, particularly differential topology, the secondary vector bundle structure refers to the natural vector bundle structure (TE,p*,TM) on the total space TE of the tangent bundle of a smooth vector bundle (E,p,M), induced by the push-forward p*:TETM of the original projection map p:EM.

In the special case (E,p,M)=(TMTM,M), where TE=TTM is the double tangent bundle, the secondary vector bundle (TTM,(πTM)*,TM) is isomorphic to the tangent bundle (TTMTTM,TM) of TM through the canonical flip.

Construction of the secondary vector bundle structure

Let (E,p,M) be a smooth vector bundle of rank N. Then the preimage (p*)-1(X)⊂TE of any tangent vector XTM in the push-forward p*:TETM of the canonical projection p:EM is a smooth submanifold of dimension 2N, and it becomes a vector space with the push-forwards

of the original addition and scalar multiplication

as its vector space operations. The triple (TE,p*,TM) becomes a smooth vector bundle with these vector space operations on its fibres.

Proof

Let (U,φ) be a local coordinate system on the base manifold M with φ(x)=(x1,...,xn) and let

be a coordinate system on E adapted to it. Then

so the fiber of the secondary vector bundle structure at XTxM is of the form

Now it turns out that

gives a local trivialization χ:TWTU×R2N for (TE,p*,TM), and the push-forwards of the original vector space operations read in the adapted coordinates as

and

so each fibre (p*)-1(X)⊂TE is a vector space and the triple (TE,p*,TM) is a smooth vector bundle.

Linearity of connections on vector bundles

The general Ehresmann connection

on a vector bundle (E,p,M) can be characterized in terms of the connector map

where vlv:EVvE is the vertical lift, and vprv:TvEVvE is the vertical projection. The mapping

induced by an Ehresmann connection is a covariant derivative on Γ(E) in the sense that

if and only if the connector map is linear with respect to the secondary vector bundle structure (TE,p*,TM) on TE. Then the connection is called linear. Note that the connector map is automatically linear with respect to the tangent bundle structure (TETE,E).

See also

References

  • P.Michor. Topics in Differential Geometry, American Mathematical Society (2008).