February this year I posted some
comments on how tensors show up in geometry. However, having enrolled in
Claudio Gorodski's course in
Riemannian Geometry at IME-USP, I now know a thing or
two about tensors I didn’t knew at the time. I’m proud to say that most of what
I said stands up to the test of time, but I would still like to make some
corrections.
If you’re interested in Riemannian geometry, I strongly recommend
Claudio’s course notes.
First and foremost, in the previous post I explicitly stated that there are
vector bundles Ei→M and F→M such that the map
that takes a tensor T∈Γ(Hom(E1⊗⋯⊗En,F)) to
the homomorphism iT:Γ(E1⊗⋯⊗En)→Γ(F) given
by (iT)(ξ1,…,ξn)p=Tp(ξp1,…,ξpn) is
not surjective. This is not the case: every C∞(M)-multilinear
map T:Γ(E1)×⋯×Γ(En)→Γ(F) is the image
of some tensor, which is to say, the value of
T(ξ1,…,ξn)p depends only on the values of
ξpi.
This result is known as the tensor field characterization lemma, and a proof
can be found in here. This particular
proof is specific to the case where each Ei=TM and
F=M×R — which is to say, the proof is specific to the case
where T:X(M)×⋯×X(M)→C∞(M) — but I believe
the same argument should work for sections of arbitrary smooth vector bundles.
The proof, however, is heavily reliant on the existence of smooth partitions of
unity, which hints at the fact that perhaps the lemma does not hold for
holomorphic vector fields over complex manifolds — i.e. perhaps there some
complex manifold X with holomorphic vector fields
Ei→X and an OX-multilinear map
T:Γ(E1)×⋯×Γ(En)→Γ(F) which is not the
image of a holomorphic tensor.
The fact that this proof is restricted to the particular case where
Ei=TM and F=M×R is not a coincidence: in most
cases we are interested in tensors with the signature X(M)×⋯×X(M)×Ω1(M)×⋯×Ω1(M)→C∞(M). The space of
tensors which take s fields and r 1-forms is usually
referred to as T(r,s)M. In particular, if
M is a Riemannian manifold with metric g, the
canonical isomorphism TpM→Tp∗M given by the metric
gp induces an isomorphism of C∞(M)-modules
X(M)→Ω1(M).
Another way to put it is to say that g induces an isomorphism
T(0,1)M→T(1,0)M,
which in turn induces the so called musical isomorphisms♯:T(s,r+1)M→T(s+1,r)M
and
♭:T(s+1,r)M→T(s,r+1)M.
In particular, T(r,s)M is canonically isomorphic
to T(0,r+s)M via ♯s, which is
the space of tensors with signature X(M)×⋯×X(M)→C∞(M) — so that the proof of the lemma for this particular case is
sufficient. That about wraps it up. Hope this helped someone 😛