Selection Rules and Light with Orbital Angular Momentum

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SUMMARY

The discussion centers on the selection rules for atomic transitions, emphasizing that electrons must change states differing in angular momentum by at most 1ħ due to the spin angular momentum of photons. However, it highlights that photons can possess arbitrary integer quantities of orbital angular momentum, suggesting that different transitions and selection rules may exist under specific conditions. The primary focus is on dipole transitions, which dominate due to the long wavelength of light compared to atomic dimensions, while transitions involving higher angular momentum exhibit significantly lower intensity. The eigenstates of light angular momentum are identified as vector spherical harmonics, with plane waves being decomposable into these states.

PREREQUISITES
  • Understanding of atomic transitions and selection rules
  • Knowledge of photon spin and orbital angular momentum
  • Familiarity with dipole transitions in quantum mechanics
  • Basic concepts of vector spherical harmonics
NEXT STEPS
  • Research the implications of orbital angular momentum in quantum optics
  • Study the mathematical framework of vector spherical harmonics
  • Explore advanced topics in dipole transitions and their applications
  • Investigate experimental techniques for observing light with orbital angular momentum
USEFUL FOR

Physicists, quantum mechanics students, optical engineers, and researchers interested in the properties of light and atomic interactions.

zen loki
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When we first learn of selection rules for atomic transitions, we learn that electrons have to change between states that differ in angular momentum by at most 1ħ, because photons have 1 unit of spin angular momentum.

However, photons can have arbitrarily high integer quantities of orbital angular momentum, meaning the total angular momentum available can be more than 1. So, would we expect that different transitions and selection rules are possible? In specific circumstances, would light with orbital angular momentum absorb differently than the same frequency without orbital angular momentum?
 
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The point is that due to the long wavelength of light as compared with atomic dimensions, by far the strongest transitions are dipole transitions. Transitions corresponding to the absorption of light with higher angular momentum have a much lower intensity. Specifically, the eigenstates of light angular momentum are the vector spherical harmonics and e.g. a plane wave can be decomposed into them.
 

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