Spherically
symmetric 1s energy eigenstate of the hydrogen atom. The electron, indicated
by the small yellow sphere, stands stationary in the field of the atomic
nucleus (no matter where it's initial position is chosen).
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Superposition
of 4p, d and f states with magnetic quantum number 0. Here again the electron
stands stationary in the field of the atomic nucleus, independently of the
chosen initial position.
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3d energyeigenstate
with magnetic quantum number 1. The electron circles about the zaxis with
constant angular velocity, independently of it's initial position.
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State with
quantum numbers n=10, l=8, m=3. Again the electrons circle about the zaxis
with constant angular velocity.
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Superposition
of the 2s and the three 2p states. The resulting probability distribution
and the Bohmian vector field are stationary.
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Nonstationary
superposition of the two eigenstates n=4, l=3, m=0 and m=2 and the eigenstate
n=5, l=2, m=1.
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Rydberg state
of the hydrogen atom. Superposition of about 150 eigenstates around n=30,
following a construction by Nauenberg (1989).
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