Applications of Invariant Theory to Quantum Physics

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SUMMARY

The discussion focuses on the applications of invariant theory of Lie Groups in quantum physics, specifically how group theory underpins the foundations of quantum mechanics. Key examples include the derivation of the Schrödinger and Pauli equations through unitary representations of the Galileo and Poincaré groups, respectively. The quantization of the spinning top illustrates the necessity of using representation theory of the rotation group for accurate descriptions. Additionally, the Wigner-Eckart theorem highlights the role of selection rules in electromagnetic transitions.

PREREQUISITES
  • Understanding of Lie Groups and their representations
  • Familiarity with quantum mechanics principles, including observables
  • Knowledge of canonical quantization techniques
  • Basic concepts of group theory in physics
NEXT STEPS
  • Explore the derivation of the Schrödinger equation using the Galileo group
  • Study the representation theory of the rotation group for quantum systems
  • Research the Wigner-Eckart theorem and its applications in quantum transitions
  • Read Hagen Kleinert's book on path integrals for practical examples of group-theoretical approaches
USEFUL FOR

Physicists, quantum mechanics students, and researchers interested in the intersection of group theory and quantum physics, particularly those looking to deepen their understanding of invariant theory applications.

timb00
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Hey everybody,

I have to give a talk in our seminar on invariant theory of Lie Groups. And I'm now looking for
easy applications of invariant theory to quantum physics. I want to present them to
motivate the discussion.

I would be lucky if someone of you has an idea where I can found examples.

Best wishes, Timb00
 
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In a sense the problem is not to find examples but to restrict yourself to interesting ones. One can treat quantum theory in its very foundations as applied (Lie-)group theory! The very definition of observables and their representation in the quantum theoretical formalism can be motivated by the application of group theory: In a sense this refines the correspondence principle of "canonical quantization" to define quantum mechanical systems by unitary (ray) representations of the corresponding symmetry group or a subgroup of it of the classical system. E.g., you can derive the Schrödinger or Pauli Equation from the demand that quantum systems live in Newtonian spacetime and thus the quantum theory should admit a unitary ray representation of the Galileo group underlying the structure of spacetime. For special relativity, the same is true for the Poincare group.

A nice example is the quantization of the spinning top, which doesn't work out right in the naive canonical quantization, but one has to use the representation theory of the rotation group to get the correct description (see, e.g., Hagen Kleinert's book on path integrals, where this is given as an example for the group-theoretical approach to quantization of classical systems).

Another application are selection rules for electromagnetic transitions, the Wigner-Eckart theorem, etc. etc. As I said, the problem is to restrict oneself to interesting examples rather than to find some :-)).
 

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