The irreducible representations of of su(2): Highest weight method

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SUMMARY

The discussion focuses on the irreducible representations of the Lie algebra su(2) using the highest weight method, specifically referencing Hall's work on page 78. Key operators defined include the raising operator π(X) and the lowering operator π(Y), with their actions on the highest weight vector u_0 clearly outlined. The relationship between the operators and the eigenvalues is established through induction, leading to the conclusion that π(X)u_{k+1} can be expressed as [(k+1)λ - (k+1)k]u_k. The discussion emphasizes the importance of Lemma 5.11 in understanding the representation structure.

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Hydaspex
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I need to understand this passage from "An Elementary Introduction to Groups and Representations" Brian C. Hall
Hi all I need to understand the following passage from Hall link page 78 :

Some notation first:

Basis for ##sl(2;C)##:

##H=\begin{pmatrix} 1&0\\0&−1\end{pmatrix} ;X=\begin{pmatrix} 0&1\\0&0\end{pmatrix} ;Y=\begin{pmatrix} 0&0\\1&0\end{pmatrix} ##

which have the commutation relations

##[H,X] = 2X ~ ~, [H,Y] =−2Y ~ , [X,Y] =H ####π(X)## acts as the raising operator such that:

##π(H)π(X)u= (α+ 2)π(X)u ##

##π(Y)## acts as the lowering operator such that:

##π(H)π(Y)u= (α−2)π(Y)u ##

There is some N≥0 such that ##π(X)^Nu \neq 0##

but ##π(X)^{N+1}u= 0 ##

We define ##u_0=π(X)^Nu ## then

##(H)u_0=λu_0##

##π(X)u_0= 0 ##
Now, by definition

##u_{k+1}=π(Y)u_k##

Using ##π(H)u_k= (λ−2k)u_k## and induction we have##π(X)u_{k+1}=π(X)π(Y)u_{k}
\\= (π(Y)π(X) +π(H))u_k
\\=π(Y) [kλ−k(k−1)]u_{k−1}+ (λ−2k)u_k
\\= [kλ−k(k−1) + (λ−2k)]u_k##I don't understand how to get ##kλ−k(k−1)]## at the third passage and why ## (λ−2k)u_k## should be zero to get

##π(X)u_{k+1}= [kλ−k(k−1)]u_k##.
 
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I have difficulties to understand how the representation is finally defined. There seem to be some mistakes in what you have written. E.g. the lines where you explain the action of ##\pi(X)## is actually the description of ##\pi(H)##, which leaves ##\pi(X).u## invariant. And I do not see where ##k^2## comes from, and ##(\lambda - 2k)u_k## isn't zero, why should it be?

I hope I gave a better description of the theorem here:
https://www.physicsforums.com/insights/lie-algebras-a-walkthrough-the-representations/
 
please read page 77 of the pdf at the link...the full proof is laid out... the theorem is clear and I don't see mistakes yet that passage to prove the lemma is obscure. Wikipedia refers to that book...https://en.wikipedia.org/wiki/Representation_theory_of_SU(2) ...
"Weights and the structure of the representation"
 
So the key is Lemma 5.11. I will omit the ##\pi## and write shortly ##\pi(X)(v)=X.v##.

As always, let us list what we have:
##u_0:=X^N.u## such that ##H.u_0=\lambda u_0=(2N+\alpha)u_0## and ##X.u_0=0\,.##
##u_k:=Y^k.u_0## and thus ##H.u_k=(\lambda-2k)u_k\,.##

The only equation which is used repeatedly is ##A.B.v=[A,B].v+B.A.v## where ##[A,B]=C## is known, so ##A.B.v=C.v+B.A.v## This is the general procedure. In Lemma 5.11. we want to know, what ##X.u_k## is.

##X.u_0 = 0## per definition of ##u_0\,.##
## X.u_1=X.Y^1.u_0= [X,Y].u_0+Y.X.u_0= H.u_0+Y.0=\lambda u_0 \,.##
Now per induction we have
\begin{align*}
X.u_{k+1}&=X.Y^{k+1}.u_0 =X.Y.(Y^k.u_0)=[X,Y].(Y^k.u_0) +Y.X.(Y^k.u_0)\\
&=H.Y^k.u_0+Y.(X.Y^k.u_0)=H.u_k+Y.(X.u_k)\\&=(\lambda-2k)u_k+[k\lambda-k(k-1)]Y.u_{k-1}\\
&=\left(\lambda - 2k + k \cdot \lambda - k^2 +k\right)u_k\\&=\left[(k+1)\lambda - k^2 - k\right]u_k\\
&=\left[(k+1)\lambda - (k+1)k\right]u_k
\end{align*}
 
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It was so obvious...Thank you for your help and I will read your insight.
 
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