Zeeman Splitting, Paschen-Back Effect

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The discussion revolves around calculating the strength of an applied magnetic field based on the observed sodium resonance lines at specific wavelengths. The user attempts to apply the formula E = (m_l + 2m_s) B μ_B but encounters an issue with obtaining an excessively large value for B. They correctly identify the transitions involved and the change in wavelength (∆λ) but seem to miscalculate the parameters leading to the incorrect field strength. The community is asked for assistance in identifying the error in the calculation process. Clarification on the application of the Paschen-Back effect in strong magnetic fields is sought to resolve the confusion.
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Homework Statement



In a very strong applied field the sodium resonance lines is foudn to have components at 588.5 nm, 589 nm and 590.1 nm. What is the strength of the applied field?


The Attempt at a Solution



So I have:

3P_(1/2) --> 3S_(1/2)

AND

3P_(3/2) ---> 3S_(1/2)


Then I know, for strong magnetic fields:

E = (m_l + 2m_s ) B μ_B

I found the max change in (m_l + 2m_s ) to be about 2 and the change in E to be hc/∆λ and I know ∆λ is 0.8 nm :

If I put all this into the equation I get B to be very large, which is clearly wrong..what I am I doing wrong?


Thanks.
 
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