Specific proof of the Riemann tensor for FRW metric

In summary, the given problem requires proving the expression Rijkl= k/R2 * (gik gjl-gil gjk) for a 3 metric gik and K=0,+1,-1. This can be derived using the Christoffel symbol definition and the Riemann tensor definition, but it is easier to do so using Killing vectors for maximally symmetric space. For the FRW universe, the same expression holds true, but it is more challenging to derive it without using Killing vectors and only using the definitions of the Christoffel symbols and Riemann tensors.
  • #1
Chromatic_Universe
Gold Member
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Homework Statement


Prove Rijkl= k/R2 * (gik gjl-gil gjk) where gik is the 3 metric for FRW universe and K =0,+1,-1, and i,j=1,2,3, that is, spatial coordinates.
.

Homework Equations


The Christoffel symbol definition:
Γμνρ = ½gμσ(∂ρgνσ+∂νgρσ-∂σgνρ)
and the Riemann tensor definition:
Rμνσρ = ∂σΓμρν-∂ρΓμσνμσλΓλρνμρλΓλσν
and the FRLW metric, in the section:
Reduced-circumference polar coordinates (under general metric section)

The Attempt at a Solution


I cannot come to the general expression for the Christoffel symbols using g_ij. But the expression can be derived using Killing vectors for maximally symmetric space. For the FRW universe(homogeneous and isotropic), the same holds true, but I am finding it difficult to get to this expression without using Killing vectors, only using the definition of Christoffel symbols and Riemann tensors.
 
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  • #2
Chromatic_Universe said:

Homework Statement


Prove Rijkl= k/R2 * (gik gjl-gil gjk) where gik is the 3 metric for FRW universe and K =0,+1,-1
.

Homework Equations


The Christoffel symbol definition and the Riemann tensor definition

The Attempt at a Solution


I cannot come to the general expression for the Christoffel symbols using g_ij.

Well, to get started, can you write down the metric, and the definition of the Christoffel symbols and Riemann tensors? You have to show some work.
 
  • #3
stevendaryl said:
Well, to get started, can you write down the metric, and the definition of the Christoffel symbols and Riemann tensors? You have to show some work.
Edited the question! Thanks!
 

Related to Specific proof of the Riemann tensor for FRW metric

1. What is the FRW metric?

The Friedmann–Lemaître–Robertson–Walker (FRW) metric is a mathematical description of the expanding universe in general relativity. It describes the curvature and geometry of the universe and is the basis for the standard model of cosmology.

2. What is the Riemann tensor?

The Riemann tensor is a mathematical object that describes how spacetime is curved in the theory of general relativity. It contains information about the curvature of spacetime and is used to calculate the gravitational effects of matter and energy.

3. Why is there a need for a specific proof for the Riemann tensor in the FRW metric?

The FRW metric is a specific case of the more general metric used in general relativity. Therefore, a specific proof is needed to show how the Riemann tensor is calculated for this specific case.

4. What is the significance of proving the Riemann tensor for the FRW metric?

Proving the Riemann tensor for the FRW metric is important because it allows for the calculation of the gravitational effects in the expanding universe model. This is crucial in understanding the evolution of the universe and making predictions about its future.

5. What is the process of proving the Riemann tensor for the FRW metric?

The proof involves using the FRW metric and the equations of general relativity to calculate the components of the Riemann tensor. This is a complex mathematical process that requires knowledge of differential geometry and tensor calculus.

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