How Do Commutation Relations Fit into the Concept of a Lie Algebra?

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SUMMARY

The discussion centers on the relationship between commutation relations and Lie algebras, specifically how generators of a Lie group, represented by the composition [A,B]=ifB, form the basis of a vector space. The commutation relations indicate the simultaneous measurability of entities and are crucial for understanding the algebraic structure. The Killing form serves as a metric for the Lie algebra, with implications for its properties based on whether the algebra is semi-simple or generates a compact Lie group.

PREREQUISITES
  • Understanding of Lie groups and Lie algebras
  • Familiarity with commutation relations in quantum mechanics
  • Knowledge of the Killing form and its properties
  • Basic concepts of unitary operators and Hermitian generators
NEXT STEPS
  • Study the properties of the Killing form in Lie algebras
  • Explore the implications of semi-simple Lie algebras
  • Investigate the role of unitary operators in quantum mechanics
  • Learn about the structure and classification of compact Lie groups
USEFUL FOR

This discussion is beneficial for mathematicians, physicists, and students studying quantum mechanics, particularly those interested in the algebraic structures underlying symmetries in physics.

Physiana
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After reading some threads I decided to post my question, since I couldn't find an sufficient answer.
In general the generators of a lie group combined with the compostion [A,B]=ifB build a Lie-Algebra. Where the Generators build the base of the vectorspace.
In a common vectorspace you can find a orthonormalbase, and the scalarproduct defines the metrik. How does the comutation relations fit in this concept? I know that the comutation relations show if two entities can be measured together with any accuracy, but what is their meaning referring to the understanding of a algebra?
I have the feeling I disorganised the whole concept...
 
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When you transform your state vectors you use unitary operators, which are expressed as exponentials of Hermitian generators. All these operators represent together a set of space-time symmetries (rotation, displacement in time and space, velocity along an axis), which form a group. Now you can multiply these group elements, and to check if the commute you expand to small order and look how the generators behave to each other, if they commute. These form Lie Algebras.
 
Physiana said:
After reading some threads I decided to post my question, since I couldn't find an sufficient answer.
In general the generators of a lie group combined with the compostion [A,B]=ifB build a Lie-Algebra. Where the Generators build the base of the vectorspace.
In a common vectorspace you can find a orthonormalbase, and the scalarproduct defines the metrik. How does the comutation relations fit in this concept? I know that the comutation relations show if two entities can be measured together with any accuracy, but what is their meaning referring to the understanding of a algebra?
I have the feeling I disorganised the whole concept...

A Lie algebra' s Killing form is used to define a metric on the algebra. If the algebra is semi-simple, the metric is non-degenerate. If the algeba generates a compact Lie group, the metric is definite.
 

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