[Physics] Index Manipulation and Angular Momentum Commutator Relations

commutatorlaplace-runge-lenz-vectoroperatorsquantum mechanics

I have been trying for hours and cannot figure it out. I am not asking anyone to do it for me, but to understand how to proceed.

We have the relations
$$[L_i,p_j] ~=~ i\hbar\; \epsilon_{ijk}p_k,$$
$$[L_i,r_j] ~=~ i\hbar\; \epsilon_{ijk}r_k,$$
$$[L_i,L_j] ~=~ i\hbar\; \epsilon_{ijk}L_k.$$

Now I am trying to calculate

$$[L_i,(p\times L)_j].$$

I do not know how to reduce it. When I try I am left with too many dummy indices that I don't know what to do. For example, using

$$[AB,C] = A[B,C]+[A,C]B,$$

and expanding the cross product in terms of Levi-Civita symbols

$$[L_i,\epsilon_{jmn}p_m L_n],$$

but I don't know how to proceed correctly from here. For example, I tried,

$$ =~ \epsilon_{jmn}(\;p_m[L_i,L_n]+[L_i,p_m]L_n ).$$

Is this correct? If so, in the next step I used the known commutation relations

$$ =~i\hbar\; \epsilon_{jmn}(\; \epsilon_{ink}p_mL_k+\epsilon_{imk}p_kL_n).$$

Once again, I am stuck and do not know how to evaluate this further. Could someone tell me what I am doing wrong, or if not, how to proceed?

Best Answer

You should use the Levi-Civita reduction formula

$$\epsilon_{ijk}\epsilon_{ilm}=\delta_{jl}\delta_{km}-\delta_{jm}\delta_{kl}$$

and using the fact that $(a\times b)_i=\epsilon_{ijk}a_jb_k$ you should be done.