Understanding Zeeman Splitting: Predicting Components in Weak Applied Fields

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SUMMARY

This discussion focuses on Zeeman splitting, specifically predicting the components produced in weak applied fields. For the normal Zeeman triplet, the transition 1D2 to 1P1 or 2P(3/2) to 2S(1/2) is identified as correct, contingent on having an even number of electrons forming a state with S=0. The sodium resonance line, originally a doublet at 589.6nm, splits into four components with a frequency difference of 2/3 Lorentz unit (LU) and six components for the 589.0nm line, with identical frequency differences.

PREREQUISITES
  • Understanding of Zeeman effect and its implications in atomic transitions.
  • Familiarity with sodium's resonance lines and their spectral characteristics.
  • Knowledge of quantum numbers and selection rules, particularly the transition rule Δm = +1, 0, -1.
  • Basic grasp of Lorentz units (LU) in the context of spectral line splitting.
NEXT STEPS
  • Study the detailed mechanics of the Zeeman effect in various atomic systems.
  • Explore the calculation of Lande g-factor for multi-electron atoms.
  • Investigate the implications of weak vs. strong magnetic fields on atomic transitions.
  • Learn about the application of quantum mechanics in predicting spectral line behavior.
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Physicists, particularly those specializing in atomic physics, students studying quantum mechanics, and researchers focused on spectroscopy and magnetic field interactions with matter.

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Homework Statement



(Q1) Which transition will produce a normal zeeman triplet in a weak applied field?


(Q2) The sodium resonance line is a doublet. What is the total number of components that appear when the line is split by a weak applied field?


The Attempt at a Solution



(Q1) 1D2 --> 1P1 or 2P(3/2) ---> 2S(1/2) ?
 
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q1. Seems correct - remember you can't shift between states with the same l-number.
 
The visual effect above is awful, sorry.

1. Sufficient and neccesary conditions for normal Zeeman triplet is:

The total number of electrons is even, and the electrons form the state with S=0, 2S+1=1.

2. As to the famous sodium doublet, the 589.6nm line will split into four lines, with frequency difference 2/3 Lorentz unit (LU), 3/4 LU, 2/3 LU, respectively; the 589.0nm line splits into six ones, with identical frequency difference of 2/3 LU. No line exists at the initial location any more.

Comments:

1. Sodium Doublet: 589.6nm: 2P_(3/2) ----->2S_(1/2), 589.0nm: 2P_(1/2) ----->2S_(1/2).

2. Transition Rule: \Delta m = +1, 0, -1.

589.0nm: 2P_(1/2) ----->2S_(1/2), m, mg

---|----------------------------------------------------- 3/2, 2
---|---------|----|-------------------------------------- 1/2, 2/3
---|---------|----|---------|----|---------------------- -1/2, -2/3
---|---------|----|---------|----|----------|----------- -3/2, -2
1 1 1 1 1 1
1 1 1 1 1 1
1 1 1 1 1 1
---|---------|----|---------|----|----------|----------- 1/2, 1
------------------|--------------|----------|----------- -1/2, -1



589.6nm: 2P_(1/2) ----->2S_(1/2), m, mg

---|---------------------------------------------------- 1/2, 2/3
---|---|-----------------|----|------------------------- -1/2, -2/3
1 1 1 1
1 1 1 1
1 1 1 1
---|---|-----------------|----|-------------------------- 1/2, 1
-------|----------------------|-------------------------- -1/2, -1


where $g$ above is Lande g fractor, and for effectively mono-electron atoms, such as 1H, 3Li, 11Na, 19K, 29Cu, 47Ag, 79Au,

3 1 S * (S+1) -- L * (L+1)
g = --- + --- (---------------------------------)
2 2 J * (J+1)
 
Last edited:

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