Internal magnetic field experienced by H atom Electron

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SUMMARY

The discussion focuses on calculating the internal magnetic field experienced by the electron in a hydrogen atom, specifically related to the 21 cm spectral line. The calculated magnetic field B was found to be 0.051 T, which contradicts Arthur Beiser's assertion that the ground state hydrogen atom should have a magnetic field of approximately 14 T. The discrepancy arises from different interpretations of the contributions to the magnetic field, particularly the distinction between spin-spin coupling and spin-orbit coupling. The 21 cm line results from hyperfine structure, not spin-orbit interaction, as the 1s state lacks orbital angular momentum.

PREREQUISITES
  • Quantum mechanics principles, particularly regarding electron spin and magnetic fields.
  • Understanding of hyperfine structure in atomic physics.
  • Familiarity with the equations of energy levels in quantum states.
  • Knowledge of the relationship between frequency, wavelength, and energy (E = hf).
NEXT STEPS
  • Study the derivation of hyperfine structure in hydrogen atoms.
  • Learn about the implications of spin-spin coupling versus spin-orbit coupling in atomic physics.
  • Explore the calculations involved in determining magnetic fields in quantum systems.
  • Investigate the significance of the 21 cm line in astrophysics and cosmology.
USEFUL FOR

Students and researchers in quantum mechanics, atomic physics, and astrophysics, particularly those interested in the magnetic properties of hydrogen and the implications of hyperfine structure.

Bosley
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Homework Statement


A 21 cm spectral line corresponds to the flipping of the electron in a hydrogen atom from having its spin parallel to the spin of the proton to having it anti-parallel. Find the internal magnetic field experienced by the electron in the hydrogen atom.


Homework Equations


lambda = 21 cm
f=c/lambda = 1.429 x 10^9 Hz
DeltaE = h f = 9.4686 x 10^-25 J

The Attempt at a Solution


According to Arthur Beiser's 1969 quantum book, the energy of an electron in a given quantum state will be higher or lower by Vm = (e*hbar/(2m))*B than its energy in the absence of the spin-orbit coupling.

I think that the DeltaE I found above would be equal to 2*Vm. Which would give me B = DeltaE*m/(e*hbar). But plugging in the numbers to that equation I get that B = .051 T.

This contradicts what Beiser says shortly thereafter, which is that the ground state hydrogen atom should have B approximately 14 T. He calculates this using B = muo*f*e/(2r) with f = 7 x 1015 where f is the number of times the hydrogen atom "sees" itself circled by the proton each second, and r = 5 x 10-11 m. I don't know why my calculation contradicts this one, and if that contradiction is ok or if I have done something wrong.

Any insight would be appreciated.
 
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The spin-orbit coupling is not responsible for the 21 cm line. The spin-orbit coupling refers to the coupling of the electrons intrinsic spin to its orbital angular momentum. Only states with nonzero orbital angular momentum are split by the spin-orbit interaction. This is one contribution to what's called fine structure of atom energy levels.

The 21 cm line is due to a splitting of the 1s state due to the coupling between the electron spin with the proton spin. The 1s state has no orbital angular momentum and there is no spin-orbit splitting for this state. The spin-spin coupling is much smaller than typical spin-orbit couplings and causes what is called hyperfine structure. I haven't checked your numbers, but it's natural to find a nuclear magnetic field that is much smaller than that due to angular momentum of the electron.
 

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