Question #145708

Write down Lx is term linear angular momentum.


Expert's answer

In classical mechanics :

L=r×pL = r\times p

Therefore to pass to quantum mechanics we just replace the physical quantities by the corresponding operators (and sometimes by "hermitianizing" the result). In rr representation we have :

L^=r^×p^=−iℏr^×∇⃗\hat{L} = \hat{r}\times\hat{p}=-i\hbar \hat{r}\times\vec{\nabla}

And so we have

L^x=−iℏ(y∂∂z−z∂∂y\hat{L}_x=-i\hbar (y\frac{\partial}{\partial z} - z\frac{\partial}{\partial y} )

We can verify that the obtained result is an observable (a hermitian operator).


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