Transformation rules for vielbein and spin connection

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The discussion centers on deriving transformation rules for vielbein and spin connection in the context of General Relativity. The user expresses confusion regarding the symbols and concepts involved, particularly the covariant derivative and the variations of vielbein and spin connection. They seek clarification and resources to better understand these topics, specifically mentioning a chapter from a textbook that provides some information. The user feels overwhelmed despite prior coursework in differential geometry. Overall, the thread highlights the challenges faced by students in grasping advanced concepts in General Relativity.
Steve Rogers
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Homework Statement
Derive the following transformation rules for vielbein and spin connection:

$$\delta e_a^\mu=(\lambda^\nu\partial_\nu e_a^\mu-e_a^\nu\partial_\nu\lambda^\mu)+\lambda_a^b e_b^\mu$$

$$\delta\omega_a^{bc}=\lambda^\mu\partial_\mu\omega_a^{bc}+(-e_a^\mu\partial_\mu\lambda^{bc}+\omega_a^{d[b}\lambda_d^{c]}+\lambda_a^d\omega_d^{bc})$$
Relevant Equations
$$[M_{ab},X_c]=X_{[a}\eta_{b]c}$$

$$[M_{ab},M^{cd}]=-\delta_{[a}^{[c}M_{b]}^{d]}=-\delta_a^c M_b^d+\delta_b^c M_a^d+\delta_a^d M_b^c-\delta_b^d M_a^c$$
I am taking a course on General Relativity. Recently, I was given the following homework assignment, which reads

> Derive the following transformation rules for vielbein and spin connection:

$$\delta e_a^\mu=(\lambda^\nu\partial_\nu e_a^\mu-e_a^\nu\partial_\nu\lambda^\mu)+\lambda_a^b e_b^\mu$$

$$\delta\omega_a^{bc}=\lambda^\mu\partial_\mu\omega_a^{bc}+(-e_a^\mu\partial_\mu\lambda^{bc}+\omega_a^{d[b}\lambda_d^{c]}+\lambda_a^d\omega_d^{bc})$$

I was instructed to use:
$$[M_{ab},X_c]=X_{[a}\eta_{b]c}$$
and
$$[M_{ab},M^{cd}]=-\delta_{[a}^{[c}M_{b]}^{d]}=-\delta_a^c M_b^d+\delta_b^c M_a^d+\delta_a^d M_b^c-\delta_b^d M_a^c.$$
Also, the professor told us to consider the covariant derivative
$$\nabla_a=e_a^\mu\partial_\mu+\frac{1}{2}\omega_a^{bc}M_{cb}$$
To be honest, I have no idea what these symbols are (after examining my GR lecture note carefully). And most frustratingly, even if I have taken a one-year course on differential geometry (mathematical rigor), I still know nothing about the covariant derivative above. What on Earth do these symbols stand for? Is there any standard textbook that can help a GR beginner like me? I came here for some advice, please. Thank you very much.
 
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Thank you. The chapter you mentioned does contain some information about vielbein, but to crack the problem, I need to find the variations of ##e_a^\mu## and ##\omega_a^{bc}##. This confuses me a lot because those ##\lambda##'s and partial derivatives in the formulas came out of nowhere.
 
At first, I derived that: $$\nabla \frac 1{\mu}=-\frac 1{{\mu}^3}\left((1-\beta^2)+\frac{\dot{\vec\beta}\cdot\vec R}c\right)\vec R$$ (dot means differentiation with respect to ##t'##). I assume this result is true because it gives valid result for magnetic field. To find electric field one should also derive partial derivative of ##\vec A## with respect to ##t##. I've used chain rule, substituted ##\vec A## and used derivative of product formula. $$\frac {\partial \vec A}{\partial t}=\frac...