Commutation relations for Spin opertors

In summary: The E field components of light are always perpendicular to the propagation vector. If you pass a beam of light through a polarizer aligned in the y direction, the only light that gets through will have its E field pointed in the y direction. You are confusing this with spin. The polarizer does not in any sense measure Sy. The E field components of light are always perpendicular to the propagation vector.
  • #1
sakkoyun
10
0
Dear physicist,

I designed an experiment for my undergraduate students. As we know, for spin operators, the commutation relation is

[Si,Sj]=ihSk

We also know, if we use two polarizers which are perpendicular each other, there is no light other side after polarizers. Namely apparatus is like,

-------------------------------------------------------------------------------------
Light source ------> 0 degree polarizer + 90 degree polarizer ------->Luxmeter (no light)
-------------------------------------------------------------------------------------

If we commute these two as,

-------------------------------------------------------------------------------------
Light source ------> 90 degree polarizer + 0 degree polarizer ------->Luxmeter (no light)
-------------------------------------------------------------------------------------

So we can say, 0 and 90 degree polarizers can commute. 0 degree polarizer may be named Sx operator and 90 degree polarizer may be named Sy operator.

According to the result of this experiment,

[Sx,Sy]=0.

Whereas [Sx,Sy]=ihSz is the rule.

Where is the problem in my mind?

Best wishes.

Serkan
 
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  • #2
Serkan, You can't identify the E-field components Ex and Ey with spin components Sx and Sy. Light is made of photons, whose spin component is always parallel or antiparallel to the propagation vector. These correspond to left- and right-handed circularly polarized waves. Linearly polarized waves are linear superpositions of the circular polarizations.
 
  • #3
Is Serkan identifying the spin and E-field components? I don't think so.

I think the important point is that, as you said, the polarization vector for light is orthogonal to the direction of propagation. If x and y are taken in the plane perpendicular to the light beam, then the z-axis points along the beam, so we have that Sz is zero, and hence there's no contradiction. (Serkan, note also the difference between mutliplying operators together, which makes no reference to states, and actually performing measurements of a real physical system!)
 
  • #4
Thank you very much for your interest. According to the results from you:

1. SxSy-SySx=0. This equation don't tell us that these operators can be commuted each other. Actually, we can not measure the polarization of the light in the z direction via the apparatus given in the first post.

2.SxSy or SySx multiplyings give pure imagine result, so we can not measure them. So we obtain SxSy=0 and SySx=0. Hence, SxSy-SySx=0-0=0.

good works,

Serkan
 
  • #5
As I thought, Serkan, you are still confused. A polarizer measures and filters the alignment of the E field. If you pass a beam of light through a polarizer aligned in the x direction, the only light that gets through will have its E field pointed in the x direction. You are confusing this with spin. The polarizer does not in any sense measure Sx.
 

1. What are spin operators?

Spin operators are mathematical operators that describe the spin of a particle in quantum mechanics. They are represented by matrices and are used to calculate the spin of a particle in different orientations.

2. What are commutation relations for spin operators?

Commutation relations for spin operators describe the relationship between different spin operators. They show how the operators interact with each other and how they can be used to calculate the spin of a particle in different directions.

3. Why are commutation relations important in quantum mechanics?

Commutation relations are important because they help us understand the behavior of particles at the quantum level. They allow us to predict the outcomes of measurements and understand the properties of particles such as spin.

4. How do commutation relations for spin operators differ from other commutation relations?

Commutation relations for spin operators are unique because they involve matrices instead of numbers. This is because spin is a quantum property and is described by matrices in quantum mechanics, unlike other physical properties that can be described by numbers.

5. Can commutation relations for spin operators be used for particles other than electrons?

Yes, commutation relations for spin operators can be used for any particle that has spin, such as protons, neutrons, and even certain types of atoms. However, the specific matrices and calculations may differ depending on the type of particle being studied.

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