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Tensor transition laws define a smooth vector bundle
Statement
For every smooth manifold and integers , the tensor-coordinate change rules define a smooth vector bundle whose fibre over is the space of type tensors on .
Facts & Assumptions
Given: A smooth manifold with overlapping charts and .
The fibre of at is the space of type tensors on (The type tensor bundle).
Tangent bases transform by the Jacobian, and cotangent bases transform by the inverse transpose Jacobian (Change-of-coordinate formula for tangent bases, Cotangent coordinate changes use the inverse transpose Jacobian).
A smooth cocycle of fibrewise linear transition maps defines a smooth vector bundle (Construction of a vector bundle from a smooth cocycle).
Proof
On a chart domain , the coordinate bases and [F1, given, construct] identify each fibre in [F1] with the fixed finite-dimensional vector space of type tensors on . This gives local trivializations
On an overlap, [L1] shows that each contravariant slot picks up one inverse [L1, step 1.1, algebra] Jacobian factor and each covariant slot picks up one Jacobian factor. Hence the tensor-coordinate change map is fibrewise linear, smooth in the base point, and satisfies the cocycle law because Jacobians and inverse Jacobians do.
Therefore [L2] applies to these local transition maps and produces a smooth [F1, L2, step 2.1] vector bundle. By construction its fibre over is the tensor space from [F1].
Thus the tensor transition laws define the smooth tensor bundle . [step 3.1]