Stupid noob question about state vectors

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Homework Help Overview

The discussion revolves around the interpretation of angular momentum eigenstates in quantum mechanics, specifically focusing on the states \(|1,-1\rangle\), \(|1,0\rangle\), and \(|1,1\rangle\) for the quantum number \(l = 1\). Participants are tasked with expressing the operators \(\hat{L}^{2}\) and \(\hat{L}_{z}\) as matrices in a three-dimensional Hilbert space.

Discussion Character

  • Conceptual clarification, Problem interpretation

Approaches and Questions Raised

  • Participants explore how to interpret the states as basis vectors in a three-dimensional Hilbert space, questioning the representation of these states in vector form. There is discussion about the ordering of the basis vectors and how to express them mathematically.

Discussion Status

Some participants have provided guidance on interpreting the states as basis vectors and suggested a conventional ordering. Others have raised further questions about the representation of states for different values of \(L\), indicating an ongoing exploration of the topic.

Contextual Notes

There is an emphasis on understanding the dimensionality of the Hilbert space, particularly how it changes with different quantum numbers, which may affect the interpretation of the states discussed.

Denver Dang
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Homework Statement


I got a Problem that says:
In this Problem we consider the angular momentum, [tex]\hat{L}[/tex], which normed common eigenstates for [tex]\hat{L}^{2}[/tex] and [tex]\hat{L}_{z}[/tex] is described by [itex]\left|l,m\right\rangle[/itex], where [itex]l[/itex] and [itex]m[/itex] is the corresponding quantum numbers:

[tex]\hat{L}^{2}\left|l,m\right\rangle = l\left(l+1\right)\hbar^{2}\left|l,m\right\rangle[/tex]

[tex]\hat{L}_{z}\left|l,m\right\rangle = m\hbar\left|l,m\right\rangle[/tex]

As usual we introduce the operators:

[tex]\hat{L}_{+} = \hat{L}_{x} + i\hat{L}_{y}[/tex] and [tex]\hat{L}_{-} = \hat{L}_{x} - i\hat{L}_{y}[/tex]

Now consider the three-dimensional subspace, [itex]\mathcal{H}[/itex], corresponding to the quantum number [itex]l = 1[/itex], ie. the states [itex]\left|1,-1\right\rangle[/itex], [itex]\left|1,0\right\rangle[/itex] and [itex]\left|1,1\right\rangle[/itex].

Now, express the operators [tex]\hat{L}^{2}[/tex] and [tex]\hat{L}_{z}[/tex] as matrices in [itex]\mathcal{H}[/itex].

Homework Equations


The Attempt at a Solution



Well, my problem is that I'm not sure how to interpret the states [itex]\left|1,-1\right\rangle[/itex], [itex]\left|1,0\right\rangle[/itex] and [itex]\left|1,1\right\rangle[/itex]. Usually when there are fx. 1 in one of them, it's the first basisvector etc. But what is it now ? Is it still a vector, in which case what kind ?
I've been flipping through my entire book to see if it showed anything similar, but I haven't been able to find anything that could tell me how I have to interpret the states "vectorwise".
So I was hoping someone could help me :)

I know it's kinda noobish, but I have been stuck here for a while, and can't seem to figure out what the matrix is before I know how to interpret the states.Regards.
 
Last edited:
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Denver Dang said:
Well, my problem is that I'm not sure how to interpret the states [itex]\left|1,-1\right\rangle[/itex], [itex]\left|1,0\right\rangle[/itex] and [itex]\left|1,1\right\rangle[/itex].
Interpret them as three basis vectors spanning a three-dimensional Hilbert space, much like i, j and k span three-dimensional Euclidean space. You can order them any way you please, but conventionally the order is |1,1>, |1,0>, |1,-1>.

I don't know if I have answered your question, but I don't understand the source of your confusion and exactly what you are asking. If you can explain exactly what troubles you, I might be able to give you a better answer.
 
Hmmm, I mean, if it was just |1> I know it would be a basis vector in three dimensions (This case at least), which I would write: (1,0,0).
But how does this look like in vector-form, that's my question and problem :)
 
Denver Dang said:
Hmmm, I mean, if it was just |1> I know it would be a basis vector in three dimensions (This case at least), which I would write: (1,0,0).
But how does this look like in vector-form, that's my question and problem :)
OK. Note that the basis states are written in the form |L,ML> where L = 1 for all three states. You can toss that out since it is the same for everybody and write the states as
|1>, |0>, |-1>. So

|1> = (1,0,0)
|0> = (0,1,0)
|-1> = (0,0,1)

:wink:
 
kuruman said:
OK. Note that the basis states are written in the form |L,ML> where L = 1 for all three states. You can toss that out since it is the same for everybody and write the states as
|1>, |0>, |-1>. So

|1> = (1,0,0)
|0> = (0,1,0)
|-1> = (0,0,1)

:wink:
Ahhh, I see :)

But what if L = 2, how would that look fx. ?
 
Denver Dang said:
Ahhh, I see :)

But what if L = 2, how would that look fx. ?
The dimensionality of the Hilbert space is n = 2*L+1. For L =2, therefore, you are in 5-dimensional Hilbert space. If you denote the basis vectors just by their ML value, you get column vectors
|2> = (1,0,0,0,0)
|1> = (0,1,0,0,0)
|0> = (0,0,1,0,0)
...
and so on.
 
kuruman said:
The dimensionality of the Hilbert space is n = 2*L+1. For L =2, therefore, you are in 5-dimensional Hilbert space. If you denote the basis vectors just by their ML value, you get column vectors
|2> = (1,0,0,0,0)
|1> = (0,1,0,0,0)
|0> = (0,0,1,0,0)
...
and so on.
Great :)

Thank you very much kuruman.
 

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