How can I calculate the expectation of L(y) using the commutation relation?

In summary, the conversation is about calculating the expectation value of the y-component of the angular momentum L, given a state |l, m>. The student is trying to prove that <L(y)> = 0 and is asking for guidance on how to approach this using the commutation relation between L(x) and L^2. They have been advised to use the raising and lowering operators and are encouraged to collaborate with another student working on the same problem.
  • #1
wam_mi
81
1

Homework Statement



I am trying to calculate the expectation of the y-component of the angular momentum L.
$<L_{y}>$. How should I approach this?


Homework Equations



I try to write it in terms of the following commutator

$L(y) = \frac{2*pi}{ih} [L_{x}, L_{z}]$


The Attempt at a Solution

 
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  • #2
What do you know about the state in which you are to take the expectation value?
 
  • #3
Avodyne said:
What do you know about the state in which you are to take the expectation value?

Hi there, the state is given as |l, m>, where l is the orbital angular momentum quantum number, and m is the magnetic moment quantum number.

I want to prove that to compute <l,m| L(y) |l,m> = <L(y)> =0, how should I approach this?

Many thanks!
 
  • #4
If I were you, I'd write [itex]L_y[/itex] in terms of the raising and lowering operators [itex]L_{\pm}[/itex]...
 
  • #5
gabbagabbahey said:
If I were you, I'd write [itex]L_y[/itex] in terms of the raising and lowering operators [itex]L_{\pm}[/itex]...

Hi there, thank you for your reply.
I was told that I have to use the commutation relation between the L(x) and L^2 to get the expectation value of L(y). How can I do that though?

Thanks
 
  • #6
wam_mi said:
Hi there, thank you for your reply.
I was told that I have to use the commutation relation between the L(x) and L^2 to get the expectation value of L(y). How can I do that though?

Thanks

I'm not sure...the only way I know of showing it is to use the raising and lowering operators.

You seem to be working on basically the exact same problem as jazznaz in this thread, so maybe you two should work together and see what you can come up with.
 

FAQ: How can I calculate the expectation of L(y) using the commutation relation?

What is angular momentum?

Angular momentum is a physical quantity that describes the rotational motion of a rigid body. It is a vector quantity that is defined as the product of an object's moment of inertia and its angular velocity. In simpler terms, it is a measure of how much an object is spinning.

How is angular momentum calculated?

The formula for calculating angular momentum is L = I * ω, where L is the angular momentum, I is the moment of inertia, and ω is the angular velocity. Moment of inertia is a measure of an object's resistance to changes in rotational motion, and angular velocity is the rate at which the object is rotating.

What is the conservation of angular momentum?

The law of conservation of angular momentum states that in a closed system, the total angular momentum remains constant. This means that the angular momentum of an object cannot change unless an external torque is applied to it. This principle is often used in understanding the motion of objects in space or in collisions.

How does angular momentum relate to rotational motion?

Angular momentum is directly related to rotational motion. As an object rotates, its angular momentum will remain constant unless a torque is applied. This means that if the object's moment of inertia decreases, its angular velocity will increase to maintain the same angular momentum, and vice versa.

What are some real-world examples of angular momentum?

There are many examples of angular momentum in everyday life. Some common examples include spinning tops, figure skaters performing spins, and the Earth rotating on its axis. In the field of astrophysics, the angular momentum of planets and stars is crucial in understanding their motion and formations. In engineering, angular momentum is also important in designing machines and structures that involve rotational motion.

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