Levi-Civita Connection: Properties and Examples

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SUMMARY

The discussion centers on the properties of the Levi-Civita connection, specifically addressing the symmetry of the connection and the differentiation of functions and one-forms on a manifold M. It is established that for any function f, the equality ##\nabla_\mu \nabla_\nu f = \nabla_\nu \nabla_\mu f## holds due to the symmetric nature of the Levi-Civita connection, represented by ##\Gamma^\alpha_{\mu \nu} = \Gamma^\alpha_{\nu \mu}##. Additionally, the confusion regarding the differentiation of one-forms is clarified, emphasizing the anti-symmetry of the wedge product and the distinction between covectors and scalars.

PREREQUISITES
  • Understanding of differential geometry concepts, particularly connections.
  • Familiarity with the Levi-Civita connection and its properties.
  • Knowledge of differential forms and the wedge product.
  • Basic calculus on manifolds, including partial derivatives and covariant derivatives.
NEXT STEPS
  • Study the properties of the Levi-Civita connection in more detail, including its role in Riemannian geometry.
  • Learn about the implications of the anti-symmetry of the wedge product in differential forms.
  • Explore the relationship between covectors and vector fields in the context of differential geometry.
  • Investigate the applications of the Levi-Civita connection in physics, particularly in general relativity.
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This discussion is beneficial for mathematicians, physicists, and students of differential geometry who are looking to deepen their understanding of connections on manifolds and their applications in theoretical contexts.

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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