Equivalent definitions of tensor field

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SUMMARY

The discussion establishes the equivalence of two definitions of a twice covariant tensor field ##T_{ab}## on a differential manifold ##M##. The first definition treats ##T_{ab}## as a smooth section of the fiber bundle formed by the tensor product of cotangent spaces ##T_p^*M \otimes T_p^*M## over each point ##p \in M##. The second defines ##T_{ab}## as a ##C^\infty(M)##-multilinear map from pairs of smooth vector fields (sections of the tangent bundle) to smooth functions on ##M##. It is clarified that the second definition must involve vector fields (tangent bundle sections), not cotangent sections, to be correct. The fiberwise tensor product construction and the use of smooth functors (as in Lee's book) rigorously justify the equivalence.

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TL;DR
About the equivalence of two different definitions of tensor field
As far as I know, there are two definitions of tensor field on a differential manifold ##M##. Just to fix ideas consider the two-times covariant tensor field ##T_{ab}## on it.

First definition: take the tensor product ##T_p^{*}M \otimes T_p^{*}M## as the fiber over the point ##p \in M## and define/build the fiber bundle over ##M##. Then ##T_{ab}## is a smooth section of such tensor product bundle on ##M##.

Second definition: given the tangent and cotangent bundles over ##M##, then ##T_{ab}## is a ##C^{\infty}##-multilinear map $$T_{ab} : \Gamma(T^{*}M) \times \Gamma(T^{*}M) \to C^{\infty}(M)$$ where ##\Gamma(T^{*}M)## is the ##C^{\infty}(M)##-module of the set of smooth sections of ##T^{*}M##.

Are the two definitions actually equivalent ?
 
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Why wouldn't they be?
 
weirdoguy said:
Why wouldn't they be?
Can you formally prove it ?
 
cianfa72 said:
TL;DR: About the equivalence of two different definitions of tensor field

As far as I know, there are two definitions of tensor field on a differential manifold ##M##. Just to fix ideas consider the two-times covariant tensor field ##T_{ab}## on it.

First definition: take the tensor product ##T_p^{*}M \otimes T_p^{*}M## as the fiber over the point ##p \in M## and define/build the fiber bundle over ##M##. Then ##T_{ab}## is a smooth section of such tensor product bundle on ##M##.

Second definition: given the tangent and cotangent bundles over ##M##, then ##T_{ab}## is a ##C^{\infty}##-multilinear map $$T_{ab} : \Gamma(T^{*}M) \times \Gamma(T^{*}M) \to C^{\infty}(M)$$ where ##\Gamma(T^{*}M)## is the ##C^{\infty}(M)##-module of the set of smooth sections of ##T^{*}M##.

Are the two definitions actually equivalent ?
The second doesn't look correct. It should be a multilinear function of sections of the tangent space, not the cotangent space.

It's helpful to just look at a vector space since fields over a bundle don't really add that much.

But for a vector space ##V## over the field ##\mathbb R##, ##V^* \otimes V^* \cong L(V, V) \rightarrow \mathbb R## where ## L(V, V) \rightarrow \mathbb R## is the space of bilinear functions on ##V##.
 
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jbergman said:
The second doesn't look correct. It should be a multilinear function of sections of the tangent space, not the cotangent space.
Oops yes, a twice covariant tensor field eats two vector fields :-)

jbergman said:
But for a vector space ##V## over the field ##\mathbb R##, ##V^* \otimes V^* \cong L(V, V) \rightarrow \mathbb R## where ## L(V, V) \rightarrow \mathbb R## is the space of bilinear functions on ##V##.
Yes, definitely.

Look now at the writing ##T^*M \otimes T^*M##. What does it refer to ?
I believe it is just a notation for the fiberwise tensor product of cotangent bundles. Indeed a (vector) fiber bundle doesn't carry any vector space structure, hence the symbol of tensor product between them is meaningless. So it basically means taking the bundle over ##M## of the fiberwise tensor product ##T^*_pM \otimes T^*_pM## for any ##p \in M##.
 
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cianfa72 said:
Oops yes, a twice covariant tensor field eats two vector fields :-)


Yes, definitely.

Look now at the writing ##T^*M \otimes T^*M##. What does it refer to ?
I believe it is just a notation for the fiberwise tensor product of cotangent bundles. Indeed a (vector) fiber bundle doesn't carry any vector space structure, hence the symbol of tensor product between them is meaningless. So it basically means taking the bundle over ##M## of the fiberwise tensor product ##T^*_pM \otimes T^*_pM## for any ##p \in M##.
Yes. In Lee's book, he defines a smooth functor with which you can lift constructions on vector spaces to vector bundles. https://en.wikipedia.org/wiki/Smooth_functor
 
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