Christoffel Symbol Ansatz for 4D Spacetime

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Discussion Overview

The discussion revolves around the formulation of the Christoffel symbols in the context of a four-dimensional spacetime metric. Participants explore the implications of the metric's structure, the dependence of the Christoffel symbols on coordinate variables, and the notation used in expressing these symbols.

Discussion Character

  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant presents an ansatz metric for four-dimensional spacetime and seeks to determine the Christoffel symbols.
  • Another participant questions the dependence of the metric components on the coordinates and suggests clarifying the notation used for the warped factor.
  • A subsequent post revises the metric to a D+1 dimensional spacetime and reiterates the need to find the Christoffel symbols.
  • There is a request for clarification on the meaning of the notation for the Christoffel symbols with two indices.
  • One participant expresses uncertainty about the notation and references a statement made by another individual regarding the relationship between different indices.
  • A request for specific references to literature or articles that use this notation is made, but it is revealed that the notation is not found in formal sources.
  • A participant shares their experience in differential geometry, noting they have not encountered Christoffel symbols with two indices, suggesting a potential misunderstanding or alternative notation.

Areas of Agreement / Disagreement

Participants express differing views on the notation and meaning of the Christoffel symbols with two indices, with no consensus reached on their interpretation or usage.

Contextual Notes

There are unresolved questions regarding the definitions and dependencies of the metric components, as well as the notation for the Christoffel symbols, which may affect the clarity of the discussion.

darida
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Ansatz metric of the four dimensional spacetime:

ds^2=a^2 g_{ab}dx^a dx^b - du^2

where:

a,b=0,1,2

a(u)=warped factor

Christoffel symbol of a three dimensional AdS spacetime:

\Gamma^{c}_{ab}= \frac{1}{2} g^{cd}(∂_b g_{da} + ∂_a g_{bd} - ∂_d g_{ba})

Now how to find \Gamma^{a}_{b}?
 
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First, what are the g_{ab}? Are they functions of the "x"s only or also of u? Clearly the Christoffel symbols depend on exactly how they depend on the coordinates. Second, what do you mean by "a(u)"? Is it that the "a" in "a^2"? You are already using "a" as an index. Surely "a(u)" is not an index so it would be better to use a different symbol.
 
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Ok I fix them:
darida said:
Ansatz metric of D+1 dimensional spacetime:

ds^2=a^2 g_{ij}dx^{i} dx^{j} + du^2

where:

Signature: - + + +

Metric g_{ij} \equiv g_{ij} (x^{i}) describes D dimensional AdS spacetime

i,j = 0,1,...,(D-1) = D dimensional curved spacetime indices

a(u) = warped factor

u = x^{D}

D = number of spatial dimensional

Christoffel symbol of D dimensional AdS spacetime:

\Gamma^{k}_{ij}= \frac{1}{2} g^{kl}(∂_{j} g_{li} + ∂_{i} g_{jl} - ∂_{l} g_{ji})

Now how to find \Gamma^{i}_{j}?
 
What does \Gamma^{i}_{j} mean, i.e., what is a \Gamma with two indices?
 
George Jones said:
What does \Gamma^{i}_{j} mean, i.e., what is a \Gamma with two indices?

I don't know that's why I asked :confused:

*edit:

Well, one said that

\Gamma^{\rho}_{\mu\nu} = ...\Gamma^{i}_{j}

R_{\mu\nu} = ...R_{ij}

where:

\mu, \nu, \rho = (D + 1) dimensional curved spacetime indices

R_{ij} = \Lambda_{D} g_{ij}

\Lambda_{D} = cosmological constant
 
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Can you give specific references? In what articles or books have you seen this notation?
 
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It's not in any articles/books. I just met someone who told me that :(
 
Just giving my two cents, but I have never seen, in my study of differential geometry, a Christoffel symbol with 2 indices. The closest I can think of would be the the connection one-forms which are a set of 6 one-forms, and so they are sometimes written with two (anti-symmetric) indices...but...that's usually written in a way different notation.
 
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Oh okay
 

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