I am in an argument with a friend from the university and we would like to clarify our problem:
We have given the following term to calculate: $$s_1 t_k \delta_{ii} \delta_{k1} \delta_{nn}$$
All indices are running from 1 to 3 (3 dimensional vectors(s,t))
My solution was the following: $$s_1 t_k \delta_{ii} \delta_{k1} \delta_{nn}$$ $$=s_1 t_k \cdot1\cdot \delta_{k1} \cdot1$$ $$=s_1 t_k \delta_{k1}$$ $$=s_1 t_1$$
However he said that the result is:
$$s_1 t_1 \cdot 3 \cdot 3$$
He did not tell me how he got the two threes but I assume it's because of the Kronecker-deltas with the same index. But as far as I see, he cannot use the sum convention by Einstein in this case.
Who got the correct solution?
But again this is about context.
Knowing only that $i,k,n$ each take one of three values, it is reasonable for the expression $s_1 t_k \delta_{ii} \delta_{nn} \delta_{k1}$ to refer to any of the following:
(1) A single one of the $27$ combinations of $i,n,k$ (2) A sum over $i$ with $n,k$ fixed; a sum over $n$ with $i,k$ fixed; a sum over $k$ with $n,i$ fixed. (3) A sum over $i,k$ with $n$ fixed. etc. etc. (4) A sum over $i,j,k$
If the interpretation is not stated explicitly, that's where notational convention comes in. I'd have assumed (4)
– Badam Baplan Dec 07 '17 at 09:30