Prove Rabcd = 0 for Space Time Metric w/ 3 Linearly Independent 4 Vector Fields

  • Thread starter Thread starter deadringer
  • Start date Start date
  • Tags Tags
    Proof
Click For Summary
SUMMARY

The discussion centers on proving that the Riemann curvature tensor, Rabcd, equals zero for a spacetime metric that allows three linearly independent 4-vector fields with vanishing covariant derivatives. The vectors are defined as (1,0,0,0), (0,1,0,0), and (0,0,1,0). The analysis reveals that the relevant Christoffel symbols are zero except for the one with both subscripts equal to 3, leading to the conclusion that the Riemann tensor must vanish under these conditions. The discussion emphasizes the importance of using a coordinate-independent definition of the Riemann tensor.

PREREQUISITES
  • Understanding of Riemann curvature tensor and its properties
  • Familiarity with covariant derivatives and Christoffel symbols
  • Knowledge of vector fields in differential geometry
  • Basic principles of general relativity and spacetime metrics
NEXT STEPS
  • Study the properties of the Riemann curvature tensor in detail
  • Learn about covariant derivatives and their applications in general relativity
  • Explore coordinate-independent definitions of geometric tensors
  • Investigate the implications of vanishing Riemann tensors in physical theories
USEFUL FOR

This discussion is beneficial for physicists, mathematicians, and students of general relativity who are exploring the geometric properties of spacetime and the implications of curvature in theoretical physics.

deadringer
Messages
32
Reaction score
0
"Show that if a space time metric admits three linearly independent 4 vector fields with vanishing covariant derivatives then Rabcd = 0"

We can set the three vectors as (1,0,0,0), (0,1,0,0) and (0,0,1,0). Use covariant derivative of vector field X^b is:

d(X^b)/d(x^a) + (Christoffel symbol with superscript b and subscripts a, c)* (X^c)

where the derivative above is partial.

Therefore the following Christoffel symbols are zero:

(superscript b, subscripts a,0)
(superscript b, subscripts a,1)
(superscript b, subscripts a,2)

Assume that the Christoffel symbols are symmetric (for a symmetric gab), therefore we know that only the Christoffel symbol with both subscripts equal to 3 can be non zero, i.e

(superscipt b, subscripts 3,3)

At this point I get stuck.
 
Physics news on Phys.org
You are being really casual about just slinging around vector components for someone who hasn't even said what the coordinate system is. You should also know by now that it's not true that any set of vector fields can be treated as corresponding to the partial derivatives of some coordinate system. (The partial derivatives commute - general vector fields don't). So stop being sloppy and use a coordinate independent definition of the Riemann tensor - one where it is defined in terms of the covariant derivative.
 

Similar threads

Replies
5
Views
4K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 24 ·
Replies
24
Views
2K
  • · Replies 11 ·
Replies
11
Views
5K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 3 ·
Replies
3
Views
6K
  • · Replies 1 ·
Replies
1
Views
4K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 19 ·
Replies
19
Views
1K