- #1
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- 483
If you put a hydrogen atom in a box (##\psi=0## on the walls of the box), spherical symmetry will be broken so ##n##,##l##,##m_l## are no longer guaranteed to be good quantum numbers. In general, the new solutions will be a linear combination of all the ##|n,l,m_l\rangle## states. I know that ##l## and ##m_l## are good quantum numbers whenever the potential or boundary conditions are spherically symmetric (only depend on the radial coordinate). I know the box boundary condition depends on both ##\theta## and ##\phi## in spherical coordinates. Is that enough to conclude that ##l## and ##m_l## no longer good quantum numbers?
The reason I'm unsure is that the act of putting a box around the hydrogen atom doesn't feel like it would torque the wavefunction (maybe shear it, but not torque it), so it seems weird that the expectation value of the angular momentum should change. So, I would expect ##\langle L^2 \rangle## to still be ##l(l+1)## and ##\langle L_z \rangle## to still be ##\hbar m_l##. Is this even possible, if the wavefunctions are a linear combination of different ##|l,m_l \rangle## states? Am I talking nonsense? Sorry!
The reason I'm unsure is that the act of putting a box around the hydrogen atom doesn't feel like it would torque the wavefunction (maybe shear it, but not torque it), so it seems weird that the expectation value of the angular momentum should change. So, I would expect ##\langle L^2 \rangle## to still be ##l(l+1)## and ##\langle L_z \rangle## to still be ##\hbar m_l##. Is this even possible, if the wavefunctions are a linear combination of different ##|l,m_l \rangle## states? Am I talking nonsense? Sorry!