Why doesn't the normal Zeeman effect produce a band?

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SUMMARY

The discussion clarifies that the normal Zeeman effect does not produce a continuous band due to the quantization of orbital angular momentum. Specifically, for a principal quantum number n, the orbital angular momentum states (L=0,1,2,...,n-1) are not split continuously; instead, the external magnetic field lifts degeneracy, allowing only specific m(L) values (-L to +L). For instance, in a p state (L=1), the allowed m(L) values are -1, 0, and +1, leading to discrete energy levels rather than a continuous spectrum.

PREREQUISITES
  • Understanding of quantum mechanics, particularly angular momentum quantization.
  • Familiarity with the Zeeman effect and its implications in atomic physics.
  • Knowledge of magnetic dipole moments and their interaction with external magnetic fields.
  • Basic grasp of vector models in quantum mechanics.
NEXT STEPS
  • Study the mathematical formulation of the Zeeman effect in quantum mechanics.
  • Explore the differences between the normal and anomalous Zeeman effects.
  • Learn about the implications of angular momentum quantization on atomic energy levels.
  • Investigate the role of external magnetic fields in altering atomic spectra.
USEFUL FOR

Physicists, students of quantum mechanics, and anyone interested in the detailed behavior of atomic systems in magnetic fields will benefit from this discussion.

quawa99
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I know that orbital angular momentum is quantized. If the potential energy is developed because of the external magnetic field applying a torque on the magnetic dipole, then from the dot product of the dipole moment and magnetic field we have a cosine term, shouldn't this give rise to all the energies corresponding to the various orientations that the orbital can have w.r.t the external magnetic field?
 
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quawa99 said:
I know that orbital angular momentum is quantized. If the potential energy is developed because of the external magnetic field applying a torque on the magnetic dipole, then from the dot product of the dipole moment and magnetic field we have a cosine term, shouldn't this give rise to all the energies corresponding to the various orientations that the orbital can have w.r.t the external magnetic field?

in normal zeeman effect the orbital angular momentum states for a particular n (principal quantum number) -which has possibility of description in states of L=0,1,2,...(n-1) which are not split normally ,the external magnetic fields lifts the degeneracy in a manner that only those m(L) values are are available /allowed with m(L) taking -L, (L-1) ...0 ,1,2 ... +L in steps of 1 only.
these are the allowed states quantum mechanically
therefore the expectation that all cos(theta) values are possible is not allowed.

For example for L=1 a p state only m(L) are -1, 0, +1 making definite theta with the z axis (magnetic field axis) in a vector model.

thereby
Considering the quantization of angular momentum , this gives equally spaced energy levels displaced from the zero field level by

z4.gif
mub.gif

so the spectrum can not be continuous and will be spaced by the above.
see; http://hyperphysics.phy-astr.gsu.edu/hbase/quantum/zeeman.html for an introductory treatment
 

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