Calculating Electron Magnetic Moment: Spin & Orbital Contributions

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SUMMARY

The discussion centers on the calculation of the electron's magnetic moment, specifically addressing the contributions from spin and orbital angular momentum. It is established that the total magnetic moment, represented as \(\mu = \gamma J\), does not equate to \(\gamma = \gamma_{spin} + \gamma_{orbital}\) due to differing g-factors for spin (S) and orbital (L) contributions. The formula for a single electron's magnetic moment is given by \({\vec\mu}=(-e/2mc)[{\vec L}+2{\vec S}]\), which leads to the derivation of the Lande g factor. The discussion emphasizes that \(\mu_J\) cannot be simply summed from \(\mu_S\) and \(\mu_L\).

PREREQUISITES
  • Understanding of angular momentum in quantum mechanics
  • Familiarity with magnetic moment calculations
  • Knowledge of the Lande g factor
  • Basic principles of magnetic resonance experiments
NEXT STEPS
  • Study the derivation of the Lande g factor in detail
  • Explore the implications of differing g-factors for spin and orbital contributions
  • Learn about magnetic resonance techniques and their applications
  • Investigate the relationship between angular momentum and magnetic moment in quantum systems
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Physicists, particularly those specializing in quantum mechanics and magnetic resonance, as well as researchers studying electron behavior in magnetic fields.

andrewm
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Say I know the total angular momentum of my electron as J. If I write the total magnetic moment as \mu = \gamma J then does \gamma = \gamma_{spin} + \gamma_{orbital} ?
 
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yes, you have one contribution from orbital motion around nucleus and one from its intrinisc spin. The g-factors and so on of course differs so one has to be careful.
 
andrewm said:
Say I know the total angular momentum of my electron as J. If I write the total magnetic moment as \mu = \gamma J then does \gamma = \gamma_{spin} + \gamma_{orbital} ?
No. Mu will not be in the direction of J, since the g factor for S and L are different.
For a single electron, {\vec\mu}=(-e/2mc)[{\vec L}+2{\vec S}].
This is the origin of the Lande g factor.
 
clem said:
No. Mu will not be in the direction of J, since the g factor for S and L are different.
For a single electron, {\vec\mu}=(-e/2mc)[{\vec L}+2{\vec S}].
This is the origin of the Lande g factor.

My research suggests one can define a \mu in the direction of J with a Lande factor

g_J= g_L\frac{J(J+1)-S(S+1)+L(L+1)}{2J(J+1)}+g_S\frac{J(J+1)+S(S+1)-L(L+1)}{2J(J+1)}

if one is measuring the total angular momentum, say in a magnetic resonance experiment. But as clem said, \mu_J \neq \mu_S + \mu_L.
 
Ok, maybe my answer was not careful enogh, what I meant with "yes" was not referring to your result \gamma = \gamma_{spin} + \gamma_{orbital}

I didn't know at what level you was asking. Sorry
 
Mu will not be in the direction of J for a single electron. The Lande g factor is for the
component of mu in the direction of J. It follows by dotting my formula for mu with J and doing some algebra, leading to Andrew's (and Lande's) formula.
 

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