Question
Show that the three commutation relations (27.14) are valid, making use of the form (27.7) for $\mathrm{L}$ and the commutation relations for the components of $\mathrm{r}$ and $\mathrm{p}$.
Step 1
7). The angular momentum operator in terms of the position vector \(\mathrm{r}\) and momentum operator \(\mathrm{p}\) is defined as: \[ \mathrm{L} = \mathrm{r} \times \mathrm{p} \] Show more…
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