Relation between affine connection and covariant derivative

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The affine connection is an operator that takes a vector and a vector field to produce a vector, while the covariant derivative is the result of applying this operator to specific vector fields. On a Lorentzian manifold, the Levi-Civita connection serves as the unique affine connection that is both symmetric and compatible with the metric, meaning the metric has a zero covariant derivative. This compatibility ensures that the covariant derivative of a vector field with respect to a vector in the tangent bundle is derived from the Levi-Civita connection. Understanding the Ricci curvature tensor as an average along all curves of parallel transports provides insight into its role in the Einstein field equations. The discussion emphasizes the importance of these mathematical concepts in the context of general relativity.
nilsgeiger
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I now study general relativity and have a few questions regarding the mathematical formulation:

1) What ist the relation between an connection and a covariant derivative?
Can you explain the exact difference?

2) One a lorentzian manifold, what ist the relation between the levi-civita-connection and the used covariant derivative?

Unrelated, but probably not important enough to justify a new thread:

3) In the einstein field equitations the ricci curvature tensor is used, the non trivial contraction of the riemann curvature tensor.
My professor told me, you can understand this as averaging along all curves of the parellel transports.
Is there an easy way to see this?
 
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nilsgeiger said:
1) What ist the relation between an connection and a covariant derivative?
Can you explain the exact difference?
The affine connection is the operator ##\nabla## that takes a vector and a vector field as input and gives a vector as result. A covariant derivative is the result ##\nabla_XY## of applying that operator to a vector field ##Y## and a vector ##X##.

At least, that's the definition used in my text: John Lee's 'Riemannian Manifolds: an Introduction to Curvature'. I daresay the exact definitions vary between writers.
 
nilsgeiger said:
2) One a lorentzian manifold, what ist the relation between the levi-civita-connection and the used covariant derivative?
If one follows the framework of my previous post, the Levi-Civita connection on a Pseudo-Riemannian manifold is the affine connection that is both symmetric and compatible with the metric. 'Compatible' has a number of different definitions, the simplest of which is that the metric must have zero covariant derivative under that connection, in every direction, everywhere in the manifold (often written as ##\nabla g\equiv 0##).

It is provable that the Levi-Civita connection is unique, ie there is only one affine connection on a Pseudo Riemannian manifold that has those two properties.

The covariant derivative of a vector field on a Pseudo-R manifold with respect to a vector in its tangent bundle will be the result of applying the Levi-Civita connection to that vector field and vector.
 
In an inertial frame of reference (IFR), there are two fixed points, A and B, which share an entangled state $$ \frac{1}{\sqrt{2}}(|0>_A|1>_B+|1>_A|0>_B) $$ At point A, a measurement is made. The state then collapses to $$ |a>_A|b>_B, \{a,b\}=\{0,1\} $$ We assume that A has the state ##|a>_A## and B has ##|b>_B## simultaneously, i.e., when their synchronized clocks both read time T However, in other inertial frames, due to the relativity of simultaneity, the moment when B has ##|b>_B##...

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