What is the Tensor Analog of the Poincare Lemma?

In summary: You can check this by solving the Hodge equation for \varphi_n. In summary, the Poincare Lemma states that every co-closed form is co-exact.
  • #1
Ancient_Nomad
15
0
Hi everyone,

I know that there is a result that corresponding to a closed p-form α, I can find a p-1 form β,
such that dβ = α.

I wanted to ask, what the tensorial analog of this would be. I mean would it be right to say that on a manifold with a lorentzian metric,

If I have a vector field A, such that

[itex]\nabla_{\mu} A^{\mu} = 0[/itex]

then there exists an anti-symmetric tensor B such that,

[itex]\nabla_{\nu} B^{\mu \nu} = A^{\mu} [/itex]

where [itex]\nabla [/itex] is the covariant derivative comaptible with the metric
(So that covariant derivative of the metric is zero)

Also, if possible, please tell me where I can find the proof of the correct statement.

Thanks in advance.
 
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  • #2
I think what you are looking for is a Poincare Lemma for the co-differential, if I get this right. So the problem is not so much about using vector fields or forms, when you have a metric available (as you say) to switch between them.

Essentially the divergence [itex]\mathrm{div}(A)[/itex] of a vector field [itex]A[/itex] is the co-differential [itex]\delta(A^{\flat})[/itex] of its corresponding one-form [itex]A^{\flat}[/itex]. As the co-differential is also nil-potent as is the exterior derivative, there is of course also a Poincare Lemma for the co-differential. Something like: Every co-closed form is co-exact.

But note that these statement generally only hold locally on manifolds with non-vanishing first Betti number.
 
  • #3
On any Riemannian manifold one has the Hodge decomposition, which states that any n-form [itex]\varphi_n[/itex] can be written

[tex]\varphi_n = d \alpha_{n-1} + \delta \beta_{n+1} + \gamma_n[/tex]
for some [itex]\alpha_{n-1}, \beta_{n+1}, \gamma_n[/itex] (the subscript indicates the degree of the form), where [itex]\delta[/itex] is the co-differential, and [itex]\gamma_n[/itex] is harmonic (i.e. [itex]d \gamma_n = \delta \gamma_n = 0[/itex]).

If we assume that [itex]\varphi_n[/itex] is co-closed, then

[tex]\delta \varphi_n = 0 = \delta d \alpha_{n-1} + 0 + 0[/tex]
hence we must have [itex]\alpha_{n-1} = 0[/itex]. If the n-th Betti number is zero, then we must also have [itex]\gamma_n = 0[/itex], and in this case [itex]\varphi_n[/itex] can be written

[tex]\varphi_n = \delta \beta_{n+1}[/tex]
This statement is always true locally.
 

FAQ: What is the Tensor Analog of the Poincare Lemma?

What is the Tensor analog of Poincare Lemma?

The Tensor analog of Poincare Lemma is a mathematical theorem that states the equivalence between cohomology and homotopy invariants for tensor fields. It is a generalization of the classical Poincare Lemma, which deals with differential forms.

What are the applications of the Tensor analog of Poincare Lemma?

The Tensor analog of Poincare Lemma has various applications in differential geometry and topology, including the study of manifolds, vector fields, and differential equations. It also has applications in theoretical physics, particularly in the field of gauge theories.

How does the Tensor analog of Poincare Lemma relate to the classical Poincare Lemma?

The Tensor analog of Poincare Lemma is a generalization of the classical Poincare Lemma. It extends the concept of differential forms to tensor fields, allowing for a more comprehensive understanding of cohomology and homotopy invariants.

Can you explain the proof of the Tensor analog of Poincare Lemma?

The proof of the Tensor analog of Poincare Lemma involves using the notion of tensor fields and their corresponding differential operators. By applying these operators to a given tensor field, one can show the equivalence between cohomology and homotopy invariants.

Are there any open problems or extensions of the Tensor analog of Poincare Lemma?

Yes, there are several open problems and extensions of the Tensor analog of Poincare Lemma. One of the main open problems is the generalization of the lemma to non-commutative algebras. Other extensions include the study of higher-order tensors and the relationship between the Tensor analog and other cohomology theories.

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