What is the Role of Magnetic Fields in Allowing Electron Transitions?

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SUMMARY

The discussion centers on the role of magnetic fields in facilitating electron transitions, specifically from the ground state (1s) to the 5d subshell of a single ionized Helium atom. It is established that energy must be supplied, likely via a photon, calculated as -E_0(1/5² - 1/1²) where E_0 = -13.6 eV. The selection rule dictates that transitions involving changes in orbital angular momentum (Δl) of 2 are not allowed; however, the introduction of a magnetic field modifies the selection rules, permitting transitions that would otherwise be forbidden. The concept of quadrupole absorption is also introduced as a method to achieve ΔL = 2.

PREREQUISITES
  • Understanding of quantum mechanics, particularly electron configurations and transitions.
  • Familiarity with angular momentum in quantum systems, including orbital (l) and spin (s) angular momentum.
  • Knowledge of selection rules governing electron transitions in atomic physics.
  • Basic principles of electromagnetism, especially the effects of magnetic fields on charged particles.
NEXT STEPS
  • Study the implications of magnetic fields on electron transitions in quantum mechanics.
  • Learn about the calculation of energy levels in hydrogen-like atoms using the Rydberg formula.
  • Explore the concept of multipole expansions in electromagnetic theory.
  • Investigate the principles of quadrupole absorption and its applications in spectroscopy.
USEFUL FOR

Students and professionals in physics, particularly those focused on quantum mechanics, atomic physics, and electromagnetism, will benefit from this discussion.

dachikid
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Hi All,

I'm a bit confused about electron transitions. I'm hoping someone will be willing to straighten me out. So the problem at hand states that a single ionized Helium atom has its single electron in the 5d shell. The z component of this electron's orbital angular momentum is [tex]\hbar[/tex] and its spin angular momentum is [tex]+\frac{1}{2}\hbar[/tex].

Now if the electron is initially in the ground state (i.e. 1s) what would be needed to get it to the 5d subshell?

So my initial thoughts are inclined to think that the electron must be given energy, possibly a photon. This energy would have a value of [tex]-E_0(\frac{1}{5^2} - \frac{1}{1^2})[/tex] where [tex]E_0=-13.6ev[/tex]

Because photons carry angular momentum, [tex]l[/tex] the orbital angular momentum of the electron must change in increments of [tex]\Delta l= \frac{+}{-}1[/tex] due in part to the "selection rule"

So a transition from a (1s) state [tex]\frac{n}{1} \frac{l}{0} \frac{m_l}{0} \frac{m_s}{\frac{+}{-}1}[/tex] to a (5d) state [tex]\frac{n}{5} \frac{l}{2} \frac{m_l}{1} \frac{m_s}{\frac{+}{-}1}[/tex] is not possible because [tex]\Delta l =2[/tex]

Now if I throw the atom in a magnetic field, the selection rule for [tex]\Delta m_l=0,\frac{+}{-}1[/tex] says the transition is allowed because [tex]\Delta m_l = +1[/tex], I think :confused:

So just introducing a magnetic field allows a transition, which is not normally allowed, to be allowed?

thanks in advanced for any help!
 
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Why not try two photons?
 
dachikid said:
So a transition from a (1s) state [tex]\frac{n}{1} \frac{l}{0} \frac{m_l}{0} \frac{m_s}{\frac{+}{-}1}[/tex] to a (5d) state [tex]\frac{n}{5} \frac{l}{2} \frac{m_l}{1} \frac{m_s}{\frac{+}{-}1}[/tex] is not possible because [tex]\Delta l =2[/tex]
[tex]\Delta L=2[/tex] is possible for quadrupole absorption.
Expand the incident EM plane wave into multipoles.
 

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