Electric dipole selection rules

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SUMMARY

The electric dipole selection rules dictate that for a transition to occur, the changes in quantum numbers must satisfy specific criteria: Δl = ±1 and Δm_l = 0, ±1. Additionally, the Wigner-Eckart theorem provides a rigorous framework for understanding these rules, indicating that the matrix element of the dipole interaction can only be non-zero when these selection rules are met. The discussion clarifies that while Δj and Δm_s are not explicitly mentioned, they are inherently related to the overall selection criteria. This understanding is crucial for analyzing atomic transitions in quantum mechanics.

PREREQUISITES
  • Understanding of quantum mechanics principles
  • Familiarity with quantum numbers (l, m_l, j, m_s, n)
  • Knowledge of perturbation theory
  • Conceptual grasp of the Wigner-Eckart theorem
NEXT STEPS
  • Study the Wigner-Eckart theorem in detail
  • Explore perturbation theory applications in quantum mechanics
  • Research the implications of electric dipole transitions in spectroscopy
  • Examine the role of selection rules in atomic and molecular physics
USEFUL FOR

Physicists, particularly those specializing in quantum mechanics, atomic physics, and spectroscopy, will benefit from this discussion on electric dipole selection rules.

yosofun
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Hi,

I am confused about the electric dipole selection rules.

Delta l = +/- 1
Delta m_l = 0, +/- 1

but are there rules for Delta j and Delta m_s and Delta n?

Is there a (semi-rigorous) way to conceptually understand selection rules?

Thanks.
 
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yosofun said:
Hi,
I am confused about the electric dipole selection rules.
Delta l = +/- 1
Delta m_l = 0, +/- 1
but are there rules for Delta j and Delta m_s and Delta n?
Is there a (semi-rigorous) way to conceptually understand selection rules?
Thanks.
Sure, there is even a completely rigorous way! It is called the Wigner-Eckart theorem, and comes from the following fact:
the dipole interaction is essentially E.x, where E is given. In first order perturbation theory, the transition probability is given by the matrix element between the initial and final state of the perturbation, so you calculate: (final | E.x |initial).
E being a constant here, you are calculating the matrix elements of x in the |n,l,m> basis, and if you realize that x is the component of a vector (a spin-1 tensorial operator), with the Wigner-Eckart theorem, you arrive at the conclusion that this matrix element can only be non-zero when the selection rules you mentionned are satisfied.
cheers,
Patrick.
 

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