For a spherical symmetric potential, the wavefunction can be expanded in terms of partial waves which is dependent on r and [tex] \theta [/tex]. How would this be possible, when the potential only depends on distance from source? Classically, there's no quantity, that could have depend even on [tex] \theta [/tex].(adsbygoogle = window.adsbygoogle || []).push({});

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# Spherical symmetric potential

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