1 Observing the normal Zeeman effect in transverse and longitudinal ...
1 Observing the normal Zeeman effect in transverse and longitudinal ...
1 Observing the normal Zeeman effect in transverse and longitudinal ...
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where α is <strong>the</strong> external angle a ray makes with <strong>the</strong> etalon (what you are measur<strong>in</strong>g) <strong>and</strong> β is <strong>the</strong><br />
<strong>in</strong>ternal angle <strong>the</strong> same ray makes <strong>in</strong>side <strong>the</strong> etalon. Equation 9 is derived from equation 8, <strong>and</strong><br />
equation 10 is Snell’s Law.<br />
Us<strong>in</strong>g <strong>the</strong>se equations calculate Δλ/λ as a function of magnetic flux density for your data. F<strong>in</strong>ally<br />
you need to convert Δλ/λ to ΔE. To do this use equation 11.<br />
∆λ<br />
∆λ<br />
∆E = − E = −hc<br />
(11)<br />
2<br />
λ λ<br />
where λ=643.8 nm for <strong>the</strong> cadmium l<strong>in</strong>e. Use your data to calculate <strong>the</strong> value of <strong>the</strong> Bohr<br />
magnetron, μB.<br />
The literature value is 57.9 μeV/T.<br />
Derivation of equation 9<br />
Any given peak has a value of k <strong>and</strong> as λ changes due to <strong>the</strong> magnetic field k rema<strong>in</strong>s constant,<br />
Therefore,<br />
∆λ<br />
2<br />
=<br />
λ<br />
∆λ<br />
=<br />
λ<br />
2 2<br />
2<br />
d n − s<strong>in</strong> α1<br />
− 2d<br />
n −<br />
⎛ n<br />
⎜<br />
⎝ n<br />
From Snell’s law<br />
2<br />
2<br />
2d<br />
n<br />
2<br />
s<strong>in</strong><br />
2<br />
− s<strong>in</strong> α ⎞ 1<br />
−1<br />
2<br />
s<strong>in</strong> ⎟<br />
− α 0 ⎠<br />
2<br />
α<br />
0<br />
s<strong>in</strong><br />
2<br />
α<br />
0<br />
s<strong>in</strong>α = ns<strong>in</strong><br />
β<br />
(14)<br />
2 2 2<br />
2<br />
2 2<br />
n s<strong>in</strong> α = n ( 1−<br />
s<strong>in</strong> β ) = n cos β<br />
(15)<br />
∆λ<br />
=<br />
λ<br />
⎛ n<br />
⎜<br />
⎝ n<br />
2<br />
2<br />
cos<br />
cos<br />
2<br />
2<br />
β ⎞ 1 cos β1<br />
⎟ −1<br />
= −1<br />
β 0 ⎠ cos β 0<br />
8<br />
(12)<br />
(13)<br />
(16)