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

jdstokes
Messages
520
Reaction score
1
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 T of the Lie algebra of SO(3) starting with the abstract commutation relations

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

He begins by defining the action of T_z,T_+ on the vector v_j by

T_z v_j = j v_j, \quad T_+ v_j = 0

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

Any help would be greatly appreciated.
 
Last edited by a moderator:
Physics news on Phys.org
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 T of the Lie algebra of SO(3) starting with the abstract commutation relations

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

He begins by defining the action of T_z,T_+ on the vector v_j by

T_z v_j = j v_j, \quad T_+ v_j = 0

but he does not explain what the v_j'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:
##\textbf{Exercise 10}:## I came across the following solution online: Questions: 1. When the author states in "that ring (not sure if he is referring to ##R## or ##R/\mathfrak{p}##, but I am guessing the later) ##x_n x_{n+1}=0## for all odd $n$ and ##x_{n+1}## is invertible, so that ##x_n=0##" 2. How does ##x_nx_{n+1}=0## implies that ##x_{n+1}## is invertible and ##x_n=0##. I mean if the quotient ring ##R/\mathfrak{p}## is an integral domain, and ##x_{n+1}## is invertible then...
The following are taken from the two sources, 1) from this online page and the book An Introduction to Module Theory by: Ibrahim Assem, Flavio U. Coelho. In the Abelian Categories chapter in the module theory text on page 157, right after presenting IV.2.21 Definition, the authors states "Image and coimage may or may not exist, but if they do, then they are unique up to isomorphism (because so are kernels and cokernels). Also in the reference url page above, the authors present two...
When decomposing a representation ##\rho## of a finite group ##G## into irreducible representations, we can find the number of times the representation contains a particular irrep ##\rho_0## through the character inner product $$ \langle \chi, \chi_0\rangle = \frac{1}{|G|} \sum_{g\in G} \chi(g) \chi_0(g)^*$$ where ##\chi## and ##\chi_0## are the characters of ##\rho## and ##\rho_0##, respectively. Since all group elements in the same conjugacy class have the same characters, this may be...
Back
Top