Angular momentum and Expectation values (Another question)

In summary, in order to calculate the expectation value of [tex]\hat{L}_x^2[/tex] in the state |l,m>, we need to use the definition of expectation value to show that [tex]\langle\hat{L}_x^2\rangle=\langle\hat{L}_x^2+\hat{L}_y^2+L_z^2\rangle=\langle\hat{L}_x^2\rangle+\langle\hat{L}_y^2\rangle+\langle\hat{L}_z^2\rangle=\langle\hat{L}_x^2\rangle+\hbar^2m^2[/tex].
  • #1
Ben4000
5
0

Homework Statement



Using the fact that ,[tex]\left\langle \hat{L}_{x}^{2} \right\rangle = \left\langle \hat{L}_{y}^{2} \right\rangle[/tex] show that [tex]\left\langle \hat{L}_{x}^{2} \right\rangle = 1/2 \hbar^{2}(l(l+1)-m^{2}.[/tex]

The Attempt at a Solution



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

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

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

[tex]\left\langle \hat{L}_{z}^{2} \right\rangle = (\hbar m)^{2}[/tex][tex]\left\langle \hat{L}^{2} \right\rangle = \left\langle \hat{L}_{x}^{2} \right\rangle + \left\langle \hat{L}_{y}^{2} \right\rangle + \left\langle \hat{L}_{z}^{2} \right\rangle[/tex]

[tex]\left\langle \hat{L}_{x}^{2} \right\rangle = 1/2 (\left\langle \hat{L}^{2} \right\rangle - \left\langle \hat{L}_{z}^{2} \right\rangle )[/tex]
I don't think that this is really showing the solution since i have just stated that

[tex]\left\langle \hat{L}^{2} \right\rangle = \left\langle \hat{L}_{x}^{2} \right\rangle + \left\langle \hat{L}_{y}^{2} \right\rangle + \left\langle \hat{L}_{z}^{2} \right\rangle[/tex]

and

[tex]\left\langle \hat{L}_{z}^{2} \right\rangle = (\hbar m)^{2}[/tex]. Unless it is genrally true that [tex]\left\langle \hat{L}^{2} \right\rangle = \left\langle \hat{L} \right\rangle^{2[/tex]
What do you think?
 
Last edited:
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  • #2
Ben4000 said:

Homework Statement



Using the fact that ,[tex]\left\langle \hat{L}_{x}^{2} \right\rangle = \left\langle \hat{L}_{y}^{2} \right\rangle[/tex] show that [tex]\left\langle \hat{L}_{x}^{2} \right\rangle = 1/2 \hbar^{2}(l(l+1)-m^{2}.[/tex]

In order to calculate any expectation value, you need to know the state of the system. I assume that you are trying to calculate [itex]\langle \hat{L}_x^2\rangle[/itex] in the state [itex]|l,m\rangle[/itex]?


I don't think that this is really showing the solution since i have just stated that

[tex]\left\langle \hat{L}^{2} \right\rangle = \left\langle \hat{L}_{x}^{2} \right\rangle + \left\langle \hat{L}_{y}^{2} \right\rangle + \left\langle \hat{L}_{z}^{2} \right\rangle[/tex]


Well, certainly [itex]\langle\hat{L}^2\rangle=\langle\hat{L}_x^2+\hat{L}_y^2+L_z^2\rangle[/itex]...What is the definition of expectation value?...Do the inner products involved satisfy properties that will allow you to conclude that [itex]\langle\hat{L}_x^2+\hat{L}_y^2+L_z^2\rangle=\langle\hat{L}_x^2\rangle+\langle\hat{L}_y^2\rangle+\langle\hat{L}_z^2\rangle[/itex]?

and

[tex]\left\langle \hat{L}_{z}^{2} \right\rangle = (\hbar m)^{2}[/tex]. Unless it is genrally true that [tex]\left\langle \hat{L}^{2} \right\rangle = \left\langle \hat{L} \right\rangle^{2[/tex]



What do you think?

Again, appeal to the definition of expectation value...
 
  • #3
gabbagabbahey said:
In order to calculate any expectation value, you need to know the state of the system. I assume that you are trying to calculate [itex]\langle \hat{L}_x^2\rangle[/itex] in the state [itex]|l,m\rangle[/itex]?

Yes

gabbagabbahey said:
Well, certainly [itex]\langle\hat{L}^2\rangle=\langle\hat{L}_x^2+\hat{L}_y^2+L_z^2\rangle[/itex]...What is the definition of expectation value?...Do the inner products involved satisfy properties that will allow you to conclude that [itex]\langle\hat{L}_x^2+\hat{L}_y^2+L_z^2\rangle=\langle\hat{L}_x^2\rangle+\langle\hat{L}_y^2\rangle+\langle\hat{L}_z^2\rangle[/itex]?
[tex] \left\langle \hat{L}^{2} \right\rangle = \left\langle l,m\right|
L^{2} \left|l,m\right\rangle
[/tex]

[tex] \left\langle l,m\right|
L^{2} \left|l,m\right\rangle = \left\langle l,m\right|
L_{x}^{2}+L_{y}^{2}+L_{z}^{2} \left|l,m\right\rangle
[/tex][tex] \left\langle l,m\right|
L^{2} \left|l,m\right\rangle = \left\langle l,m\right|
L_{x}^{2}\left|l,m\right\rangle + \left\langle l,m\right|L_{y}^{2}\left|l,m\right\rangle +\left\langle l,m\right| L_{z}^{2} \left|l,m\right\rangle
[/tex]

[tex]
\left\langle \hat{L}^{2} \right\rangle = \left\langle \hat{L}_{x}^{2} \right\rangle + \left\langle \hat{L}_{y}^{2} \right\rangle + \left\langle \hat{L}_{z}^{2} \right\rangle
[/tex]

yes?

gabbagabbahey said:
Again, appeal to the definition of expectation value...

Still not so sure about this one...

[tex]
\left\langle l,m\right| L_{z} \left|l,m\right\rangle = \hbar m
[/tex]

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

[tex]
L_{z}^{2} \left|l,m\right\rangle = (\hbar m)^{2} \left|l,m\right\rangle
[/tex]

[tex]
\left\langle l,m\right| L_{z}^{2} \left|l,m\right\rangle = (\hbar m)^{2}
[/tex]
 
  • #4
Ben4000 said:
Still not so sure about this one...

[tex]
L_{z}^{2} \left|l,m\right\rangle = (\hbar m)^{2} \left|l,m\right\rangle
[/tex]

[tex]
\left\langle l,m\right| L_{z}^{2} \left|l,m\right\rangle = (\hbar m)^{2}
[/tex]

Why aren't you sure about this?

[tex]\langle L_{z}^{2} \rangle=\left\langle l,m\right| L_{z}^{2} \left|l,m\right\rangle=\langle l,m| (\hbar m)^{2} |l,m\rangle=\hbar^2m^2\langle l,m |l,m\rangle[/tex]
 
  • #5
gabbagabbahey said:
Why aren't you sure about this?

[tex]\langle L_{z}^{2} \rangle=\left\langle l,m\right| L_{z}^{2} \left|l,m\right\rangle=\langle l,m| (\hbar m)^{2} |l,m\rangle=\hbar^2m^2\langle l,m |l,m\rangle[/tex]
I am not sure how you can infer that [tex]
\hat{L}_{z}^{2} = (\hbar m)^{2}
[/tex] from [tex]
L_{z} \left|l,m\right\rangle = \hbar m \left|l,m\right\rangle
[/tex]
 
Last edited:
  • #6
Ben4000 said:
I am not sure how you can infer that [tex]
\hat{L}_{z}^{2} = (\hbar m)^{2}
[/tex] from [tex]
L_{z} \left|l,m\right\rangle = \hbar m \left|l,m\right\rangle
[/tex]

You can't!

However, you can infer that

[tex]L_z^2|l,m\rangle=L_zL_z|l,m\rangle=L_z(\hbar m|l,m\rangle)=\hbar m L_z|l,m\rangle=\hbar^2 m^2|l,m\rangle[/itex]

and that's all that's needed.
 

1. What is angular momentum?

Angular momentum is a physical quantity that measures the amount of rotational motion of an object. It is a vector quantity that takes into account both the speed of rotation and the direction of the axis of rotation.

2. How is angular momentum calculated?

Angular momentum is calculated by multiplying the moment of inertia (the object's resistance to rotational motion) by the angular velocity (the rate of rotation). The formula for angular momentum is L = Iω, where L is angular momentum, I is moment of inertia, and ω is angular velocity.

3. What is the significance of angular momentum?

Angular momentum is an important concept in physics as it is conserved in a closed system, meaning that the total angular momentum of a system will remain constant unless an external torque is applied. It also plays a crucial role in understanding the behavior of objects in rotational motion, such as planets orbiting around a star.

4. What are the different types of angular momentum?

There are two types of angular momentum: orbital angular momentum and spin angular momentum. Orbital angular momentum refers to the rotational motion of an object around a fixed point, while spin angular momentum is the intrinsic angular momentum of a particle or object.

5. What is the relationship between angular momentum and expectation values?

In quantum mechanics, angular momentum and expectation values are closely related. The expectation value of a physical quantity, such as angular momentum, is the average value that would be obtained if the measurement was repeated multiple times. In the case of angular momentum, the expectation value is related to the quantum mechanical operator for angular momentum and can provide information about the state of a system.

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