because energy eigenstates have trivial time evolution .. if you prepare the state in some Ψnlm , then you are simply just more likely to find it in certain places than another, that's like the whole thing .. and you don't even need very exotic states to acheive this at all
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The initial question was how to represent an hydrogen atom. Drawing some orbitals gives a poor representation of an hydrogen atom in my opinion.
okay that's fine, but that's a different point and clearly different upon reading the thread, than what wood was arguing