How to Prove \(R^a_{[bcd]} = 0\) Using the Ricci Identity?

  • Thread starter Thread starter CAF123
  • Start date Start date
  • Tags Tags
    Identity
CAF123
Gold Member
Messages
2,918
Reaction score
87
1. Homework Statement
Given ##\nabla## a torsionless connection, the Ricci identity for co-vectors is $$\nabla_a \nabla_b \lambda_c - \nabla_b \nabla_a \lambda_c = -R^d_{\,\,cab}\lambda_d.$$
Prove ##R^a_{[bcd]} = 0## by considering the co-vector field ##\lambda_c = \nabla_c f##

Homework Equations


$$R^a_{[bcd]} = 0 = \frac{1}{3!} \left(R^a_{\,\,bcd} + R^a_{\,\,cdb} + R^a_{\,\,dbc} - R^a_{\,\,bdc} - R^a_{\,\,cbd} - R^a_{\,\,dcb}\right)$$

The Attempt at a Solution


Input the given form for the covector into the Ricci identity in the question. Then since ##\nabla_c f = e_c(f),## we have
$$\nabla_a \nabla_b e_c(f) - \nabla_b \nabla_a e_c(f) = -R^d_{\,\,cab}e_d(f).$$ True for all functions f, so $$\nabla_a \nabla_b e_c - \nabla_b \nabla_a e_c = -R^d_{\,\,cab}e_d.$$ Then since ##\nabla_a e_b = \Gamma^d_{ba} e_d## we can simplify the above to give $$\nabla_a \Gamma^d_{cb}e_d - \nabla_b \Gamma^d_{ca}e_d = -R^d_{\,\,cab}e_d$$ which can then be further rewritten like $$\nabla_a \Gamma^d_{cb} + \Gamma^{\alpha}_{cb}\Gamma^d_{\alpha a} - \nabla_b \Gamma^d_{ca} - \Gamma^{\alpha}_{ca}\Gamma^d_{\alpha b} = -R^d_{\,\,cab}.$$ I was then going to relabel all indices to get terms like that in the equation in 'Relevant Equations' and sum them all up and I hoped to get zero, but it is not. Have I made an error in the above somewhere? Thanks!
 
Last edited:
Physics news on Phys.org
I'm a bit rusty on this stuff, but,... since no one else has replied,...

Where did this problem come from? Is it from a textbook? Online notes? (If the latter, please provide a link.)

CAF123 said:
$$R^a_{[bcd]} = 0 = \frac{1}{3!} \left(R^a_{\,\,bcd} + R^a_{\,\,cdb} + R^a_{\,\,dbc} - R^a_{\,\,bdc} - R^a_{\,\,cbd} - R^a_{\,\,dcb}\right)$$
Since ##R^a_{bcd}## is already skewsymmetric in the last 2 indices, you can simplify the rhs down to 3 terms, which is a sum of cyclically permuted b,c,d, indices. In that form it's called the "first Bianchi identity". Proving that might be less work. Check out the associated formulas on Wikipedia.

Also, I don't understand how you went from your 2nd-last line to your last line.
 
I just realized... the correct method is sketched in Wald p39.

(I guess I'm rustier than I realized.)
 
Last edited:
Thread 'Need help understanding this figure on energy levels'
This figure is from "Introduction to Quantum Mechanics" by Griffiths (3rd edition). It is available to download. It is from page 142. I am hoping the usual people on this site will give me a hand understanding what is going on in the figure. After the equation (4.50) it says "It is customary to introduce the principal quantum number, ##n##, which simply orders the allowed energies, starting with 1 for the ground state. (see the figure)" I still don't understand the figure :( Here is...
Thread 'Understanding how to "tack on" the time wiggle factor'
The last problem I posted on QM made it into advanced homework help, that is why I am putting it here. I am sorry for any hassle imposed on the moderators by myself. Part (a) is quite easy. We get $$\sigma_1 = 2\lambda, \mathbf{v}_1 = \begin{pmatrix} 0 \\ 0 \\ 1 \end{pmatrix} \sigma_2 = \lambda, \mathbf{v}_2 = \begin{pmatrix} 1/\sqrt{2} \\ 1/\sqrt{2} \\ 0 \end{pmatrix} \sigma_3 = -\lambda, \mathbf{v}_3 = \begin{pmatrix} 1/\sqrt{2} \\ -1/\sqrt{2} \\ 0 \end{pmatrix} $$ There are two ways...
Back
Top