Levi-Civita Connection: Properties and Examples

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The discussion focuses on the properties of the Levi-Civita connection in relation to functions and one-forms on a manifold. In part (a), it is clarified that while the equality ##\nabla_\mu \nabla_\nu f = \nabla_\nu \nabla_\mu f## holds due to the symmetry of the connection, the components of the covector must be treated correctly, as they are not scalars. In part (b), the confusion arises from not accounting for the anti-symmetry of the wedge product, which leads to the vanishing of certain terms involving the connection coefficients. The participants emphasize the importance of recognizing that derivatives of functions yield covector fields rather than scalar fields. Overall, the discussion highlights the nuances of working with connections and their properties in differential geometry.
Silviu
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Homework Statement


Let V be a Levi-Civita connection.
a) Let ##f \in F(M)##, (function defined on the manifold M). Show that: ##\nabla_\mu \nabla_\nu f = \nabla_\nu \nabla_\mu f ##
b) Let ##\omega \in \Omega^1(M)## (one form on M). Show that ##d \omega = (\nabla_\mu \omega)_\nu dx^\mu \wedge dx^\nu##

Homework Equations


Levi-Civita is a symmetric connection, i.e. ##\Gamma^\alpha_{\mu \nu} = \Gamma^\alpha_{\nu \mu}##

The Attempt at a Solution


a) For any connection, function f and vector X, we have ##\nabla_X f = X[f]##. So in our case ##\nabla_\mu \nabla_nu f = \frac{\partial}{\partial x_\mu}\frac{\partial}{\partial x_\nu} f = \frac{\partial}{\partial x_\nu}\frac{\partial}{\partial x_\mu} f = \nabla_\nu \nabla_\mu f ##. Is this correct? And if so, why does the connection has to be Levi-Civita, it seems to work for any connection?

b) ##\omega = a_\nu dx^\nu##. By definition, ##d\omega = \frac{\partial a_\nu}{\partial x_\mu}dx^\mu \wedge dx^\nu##. But ##(\nabla_\mu \omega)_\nu = \frac{\partial a_\nu}{\partial x_\mu} - \Gamma^\lambda_{\mu\nu}a_\lambda##. I am a bit confused of what I did wrong here, as the 2 results don't match and ##\Gamma^\lambda_{\mu\nu}## doesn't vanish, even in a Levi Civita connection. Can someone help me? Thank you!
 
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Silviu said:
Is this correct?
No, it is not correct. ##\nabla_\nu f## is not a scalar. It is the components of a covector.

In (b) you are not taking into account that the wedge product is anti-symmetric.
 
Orodruin said:
No, it is not correct. ##\nabla_\nu f## is not a scalar. It is the components of a covector.

In (b) you are not taking into account that the wedge product is anti-symmetric.
So for part b), ##\Gamma^{\lambda}_{\mu \nu}a_\lambda dx^\mu \wedge dx^\nu## vanishes because we multiply a symmetric term with an antisymmetric term. Thank you! For part a) I am not sure I understand. Isn't ##\nabla_\nu f = \frac{\partial}{\partial x^\nu}f##, which is just the derivative of a function, which is a number, so it creates a scalar field?
 
Silviu said:
Isn't ∇νf=∂∂xνf∇νf=∂∂xνf\nabla_\nu f = \frac{\partial}{\partial x^\nu}f, which is just the derivative of a function, which is a number, so it creates a scalar field?
No.
 
Orodruin said:
No.
Then, what is the right formula for ##\nabla_\nu f##?
 
Silviu said:
Then, what is the right formula for ##\nabla_\nu f##?
For a scalar field ##\nabla_\nu f = \partial_\nu f##, but ##\partial_\nu f## is not a scalar field so generally ##\nabla_\mu \partial_\nu f \neq \partial_\mu \partial_\nu f##. Compare to the components of the gradient in regular Euclidean space.
 
Orodruin said:
For a scalar field ##\nabla_\nu f = \partial_\nu f##, but ##\partial_\nu f## is not a scalar field so generally ##\nabla_\mu \partial_\nu f \neq \partial_\mu \partial_\nu f##. Compare to the components of the gradient in regular Euclidean space.
So do you mean to treat ##\partial_\nu f## as a vector field?
 
Silviu said:
So do you mean to treat ##\partial_\nu f## as a vector field?
You should, because it is a (dual) vector field.
 
Orodruin said:
You should, because it is a (dual) vector field.
Thanks a lot!
 

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