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

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SUMMARY

The relation 0 ≤ l < n-1 for quantum numbers is crucial for understanding the angular momentum eigenvalue equation in quantum mechanics. This constraint arises from the need for convergence in the Frobenius solution, particularly in spherically symmetric systems like the hydrogen atom. The quantum number n serves as an accidental quantum number due to the extra symmetry of the hydrogen atom, leading to degeneracies in energy states. This classification allows for a systematic organization of quantum states based on radial nodes and angular momentum.

PREREQUISITES
  • Understanding of quantum mechanics principles
  • Familiarity with angular momentum quantum numbers
  • Knowledge of the Frobenius method for solving differential equations
  • Concept of degeneracy in quantum states
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  • Study the Frobenius method in detail for differential equations
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  • Research the symmetry properties of the hydrogen atom
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Students and professionals in physics, particularly those focusing on quantum mechanics, atomic physics, and anyone interested in the mathematical foundations of quantum numbers and their implications in spherically symmetric systems.

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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