Selection rules and related stuffs

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SUMMARY

The discussion focuses on selection rules in quantum mechanics, specifically regarding electric dipole transitions and their classification. It explains that selection rules arise from the conservation of quantum numbers and highlights the significance of the electric dipole operator in determining transition probabilities. The conversation also distinguishes between various types of transitions, including dipole-dipole, magnetic-dipole, electric quadrupole, and magnetic quadrupole transitions. A comprehensive understanding of why certain matrix elements are zero requires knowledge of group theory.

PREREQUISITES
  • Quantum mechanics fundamentals
  • Understanding of quantum numbers
  • Familiarity with dipole transitions
  • Basic group theory concepts
NEXT STEPS
  • Study electric dipole transitions in detail
  • Explore the role of group theory in quantum mechanics
  • Learn about magnetic dipole and electric quadrupole transitions
  • Investigate matrix elements and their significance in atomic transitions
USEFUL FOR

Students and professionals in physics, particularly those specializing in quantum mechanics, atomic physics, and spectroscopy, will benefit from this discussion.

Weimin
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I'm quite confuse with some concepts here.

The selection rules are derived from the requirements that quantum numbers must be conserved. It's OK. Then I see they give rules for so-called electric dipole transitions. I just wonder why dipole comes in here. How do you classify these kinds of transitions:

1. An electron absorbs a photon and then jumps to the higher level.

2. In magnetic resonance, if we apply an rf with energy match to the separation between two energy levels, the electron spin can flip. The difference to case 1 is we have magnetic field involved.

Can you give me the examples of dipole-dipole, magnetic-dipole, electric quadrupole, magnetic quadrupole, quadrupole transitions? Is there any way to understand the selection rules rather than remember the table of selection rules?
 
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In semi-classical approximation of matter-light interaction, the atomic system (the matter) is quantized while the light is treated as a classical field. In that approximation, the probability for the atomic system to excite/deexcite is proportional to something like a series of matrix elements of certain operators between the initial and final states of the atomic system. The selection rules state when those matrix elements could be non-zero. The main term in the series is the electric dipole operator which gives rise to dipole transition rules. If that matrix element is zero, the probability for atomic transition is severely decreased, yet you have weaker operators in the series, like magnetic dipole, electric quadrupole etc. that can have non-zero matrix elements and still cause transition. Weaker transitions will show as fainter lines in the experimental atomic spectrum.

A full understanding why the matrix elements of a given operator between two sates are zero can be achieved only after you learn group theory.
 
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Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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