Why is the relation 0 ≤ l < n-1 for quantum numbers important?

Gavroy
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hey,

i asked myself, how one could derive the relations for the quantum numbers...
so why is:
l always: 0<l<n-1
from what follows this relation for l
does anyone know this?
 
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I believe 0<l<n-1 for convergence of the Frobenius solution to the angular momentum eigenvalue equation.
 
Gavroy said:
hey,

i asked myself, how one could derive the relations for the quantum numbers...
so why is:
l always: 0<l<n-1
from what follows this relation for l
does anyone know this?

Yes, the "reason" is that n is an accidental quantum number in a sense, because the hydrogen atom has an extra symmetry that makes lots of states degenerate which you wouldn't expect them to be.

For any spherically symmetric problem, the obvious quantum numbers to use are the number of radial nodes, and then the angular momentum quantum numbers. Imagine a piece of graph paper with number of radial nodes along the x-axis, and angular momentum quantum number along the y-axis. Then at every position with non-negative integer coordinates there are (2l+1) degenerate states. Then you have a nice classification of all states of hydrogen, labial by the number of radial nodes, and the angular momentum.

The extra symmetry of hydrogen means that states on diagonals are degenerate, and so the energy quantum number is an equivalent way to label the states, but the n quantum number is constrained since (#radialnodes+ l +1 = n).
 
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If we release an electron around a positively charged sphere, the initial state of electron is a linear combination of Hydrogen-like states. According to quantum mechanics, evolution of time would not change this initial state because the potential is time independent. However, classically we expect the electron to collide with the sphere. So, it seems that the quantum and classics predict different behaviours!
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