词条 | Secondary vector bundle structure |
释义 |
In mathematics, particularly differential topology, the secondary vector bundle structure refers to the natural vector bundle structure {{math|(TE, p∗, TM)}} on the total space TE of the tangent bundle of a smooth vector bundle {{math|(E, p, M)}}, induced by the push-forward {{math|p∗ : TE → TM}} of the original projection map {{math|p : E → M}}. This gives rise to a double vector bundle structure {{math|(TE,E,TM,M)}}. In the special case {{math|(E, p, M) {{=}} (TM, πTM, M)}}, where {{math|TE {{=}} TTM}} is the double tangent bundle, the secondary vector bundle {{math|(TTM, (πTM)∗, TM)}} is isomorphic to the tangent bundle {{math|(TTM, πTTM, TM)}} of {{math|TM}} through the canonical flip.Construction of the secondary vector bundle structureLet {{math|(E, p, M)}} be a smooth vector bundle of rank {{mvar|N}}. Then the preimage {{math|(p∗)−1(X) ⊂ TE}} of any tangent vector {{mvar|X}} in {{math|TM}} in the push-forward {{math|p∗ : TE → TM}} of the canonical projection {{math|p : E → M}} is a smooth submanifold of dimension {{math|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 {{math|(TE, p∗, TM)}} becomes a smooth vector bundle with these vector space operations on its fibres. ProofLet {{math|(U, φ)}} be a local coordinate system on the base manifold {{mvar|M}} with {{math|φ(x) {{=}} (x1, ..., xn)}} and let be a coordinate system on adapted to it. Then so the fiber of the secondary vector bundle structure at {{mvar|X}} in {{math|TxM}} is of the form Now it turns out that gives a local trivialization {{math|χ : TW → TU × R2N}} for {{math|(TE, p∗, TM)}}, and the push-forwards of the original vector space operations read in the adapted coordinates as and so each fibre {{math|(p∗)−1(X) ⊂ TE}} is a vector space and the triple {{math|(TE, p∗, TM)}} is a smooth vector bundle. Linearity of connections on vector bundlesThe general Ehresmann connection {{math|TE {{=}} HE ⊕ VE}} on a vector bundle {{math|(E, p, M)}} can be characterized in terms of the connector map where {{math|vlv : E → VvE}} is the vertical lift, and {{math|vprv : TvE → VvE}} is the vertical projection. The mapping induced by an Ehresmann connection is a covariant derivative on {{math|Γ(E)}} in the sense that if and only if the connector map is linear with respect to the secondary vector bundle structure {{math|(TE, p∗, TM)}} on {{math|TE}}. Then the connection is called linear. Note that the connector map is automatically linear with respect to the tangent bundle structure {{math|(TE, πTE, E)}}. See also
References
3 : Differential geometry|Topology|Differential topology |
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