What are the v_j vectors in Cahn's representation of the Lie algebra of SO(3)?

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SUMMARY

The discussion centers on the representation of the Lie algebra of SO(3) as presented in Cahn's book on semi-simple Lie algebras. Specifically, it addresses the (2j+1)-dimensional representation T, defined by the commutation relations [T_z,T_+] = T_+, [T_z,T_-] = -T_-, and [T_+,T_-] = 2T_z. The vectors v_j are introduced in the context of the actions T_z v_j = j v_j and T_+ v_j = 0, but their existence and definition are not clarified in the text. Participants seek to understand the nature and significance of these vectors in the representation theory.

PREREQUISITES
  • Understanding of Lie algebras, specifically the structure of SO(3).
  • Familiarity with representation theory in quantum mechanics.
  • Knowledge of commutation relations and their implications in quantum physics.
  • Basic concepts of dimensionality in vector spaces.
NEXT STEPS
  • Study the representation theory of Lie algebras, focusing on SO(3) and its applications.
  • Explore the concept of weight vectors in the context of Lie algebra representations.
  • Review Cahn's book on semi-simple Lie algebras for deeper insights into the definitions and properties of v_j vectors.
  • Investigate the mathematical foundations of quantum mechanics that relate to angular momentum and its representations.
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Quantum physicists, mathematicians specializing in representation theory, and students studying the algebraic structures in quantum mechanics will benefit from this discussion.

jdstokes
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Hi all, I asked this on the Quantum Physics board but didn't get a response.

I'm reading Cahn's book on semi-simple lie algebras and their representations.

http://www-physics.lbl.gov/~rncahn/book.html

In chapter 1, he attempts to build a (2j+1)-dimensional representation [itex]T[/itex] of the Lie algebra of SO(3) starting with the abstract commutation relations

[itex][T_z,T_+] = T_+, \quad [T_z,T_-] = - T_-,\quad [T_+,T_-] = 2T_z[/itex] Eq (I.14).

He begins by defining the action of [itex]T_z,T_+[/itex] on the vector [itex]v_j[/itex] by

[itex]T_z v_j = j v_j, \quad T_+ v_j = 0[/itex]

but he does not explain what the [itex]v_j[/itex]'s are. How does one even know that such vectors exist?

Any help would be greatly appreciated.
 
Last edited by a moderator:
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jdstokes said:
Hi all, I asked this on the Quantum Physics board but didn't get a response.

I'm reading Cahn's book on semi-simple lie algebras and their representations.

http://www-physics.lbl.gov/~rncahn/book.html

In chapter 1, he attempts to build a (2j+1)-dimensional representation [itex]T[/itex] of the Lie algebra of SO(3) starting with the abstract commutation relations

[itex][T_z,T_+] = T_+, \quad [T_z,T_-] = - T_-,\quad [T_+,T_-] = 2T_z[/itex] Eq (I.14).

He begins by defining the action of [itex]T_z,T_+[/itex] on the vector [itex]v_j[/itex] by

[itex]T_z v_j = j v_j, \quad T_+ v_j = 0[/itex]

but he does not explain what the [itex]v_j[/itex]'s are. How does one even know that such vectors exist?

Any help would be greatly appreciated.

[EDIT]I've decided to answer on the quantum physics forum[/EDIT]
 
Last edited by a moderator:

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