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Science · Advanced Physics
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In this exercise we consider a hydrogen atom (spin and fine stricture is neglected). The normalized eigenfunctions are Where n is the principle quantum number, and / and m are the usual quantum numbers belongingg to 13 and L: respectivly. As usual use the operators + iL a) Show that ntm() is an eigenfunction for the operator LLand find the eigenvalue b) Consider the state: 21-1(7 Show that an eigenfunction for the energy as for i2, but not L.

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