How Does Tensor Notation Work in Group Theory Calculations?

christodouloum
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1. While reading notes on group theory there is a step I could not reproduce although it seems to me it should be straightforward. Probably there is something I am missing on tensor indices notation. Since R is an orthogonal matrix you can...

2 ...go from \epsilon _{lmn}R_{il}R_{jm}R_{kn}=\epsilon_{ijk}

to \epsilon_{lmn}R_{jm}R_{kn}=\epsilon_{ijk}R_{il}


3. Since R is orthogonal I wrote down R_{il}R_{ir}=\delta _{lr}. So I multiply both sides by R_il and by relabelling r with l it works. But can I do that?
 
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Indices are dummy tokens; they could be pink hearts, orange stars, yellow moons, et cetera. You can always rename one index letter to another as long as you do so consistently throughout the entire expression or equation.
 
There are two things I don't understand about this problem. First, when finding the nth root of a number, there should in theory be n solutions. However, the formula produces n+1 roots. Here is how. The first root is simply ##\left(r\right)^{\left(\frac{1}{n}\right)}##. Then you multiply this first root by n additional expressions given by the formula, as you go through k=0,1,...n-1. So you end up with n+1 roots, which cannot be correct. Let me illustrate what I mean. For this...
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