The following is an excerpt from Prof David Tong's notes on Classical Dynamics. This is in the section on Kinematics:
I am unable to understand how the equation circled in red, is the same as the condition for an orthogonal matrix given after 'in other words.' I may be missing something obvious, but I'm not sure what it is. What I have tried is the following:
$$R_{ac}R_{bc} = \delta_{ab} \implies R_{ac}R_{cb}^T = \delta_{ab} \implies RR^T = I$$
But how does this guarantee that $R^TR = I$ ?
Further, for two matrices $A_{m\times n}$ and $B_{n\times l}$ the product in index notation is given by:
$$(AB)_{ml} = \sum_n A_{mn}B_{nl}$$
For a general square matrix M, the condition on it being orthogonal is that:
$$M^TM = MM^T = I$$ If I try to write the first condition in index notation I seem to get:
$$(M^TM)_{jj} = \sum_iM_{ji}M_{ij}$$
But how do I get the non diagonal elements of this product at all? Do I change the index on one of the matrices?
Throughout the rest of this section wherever I expect a certain index ordering, I find that he has written down the opposite (for example here, I think it should be $R_{ac}R_{cb} = \delta_{ab}$) so I think there is something I don't understand with the notation, or something more fundamental that I am missing.