Is the Pauli-Lubanski Vector Always Zero?

In summary, the conversation discusses the identity J^{ab}P^c + J^{bc}P^a+J^{ca}P^b = 0 and its application to the Pauli-Lubanski vector. It is noted that the identity can be proven faster by noticing that certain partial derivatives commute. However, this only applies to a spin-0 particle and things are different for particles with non-zero intrinsic spin.
  • #1
tamiry
10
0

Homework Statement


Hi
i've noticed that,
[tex]J^{ab}P^c + J^{bc}P^a+J^{ca}P^b = 0[/tex]
[
Since
[tex]J^{ab}P^c + J^{bc}P^a+J^{ca}P^b = x^a\partial^b\partial^c -x^b\partial^a\partial^c + x^b\partial^c\partial^a-x^c\partial^b\partial^a+x^c\partial^a\partial^b-x^a\partial^c\partial^b = 0[/tex]
]

Next, I tried it on the Pauli Lubanski vector. Suppose I'll look at W0 as an example
[tex]W_x = (1/2)\epsilon_{xabc}J^{ab}P^c [/tex]
[tex]2W_0 = \epsilon_{0abc}J^{ab}P^c = \epsilon_{0123}J^{12}P^3+\epsilon_{0132}J^{13}P^2+\epsilon_{0231}J^{23}P^1+\epsilon_{0213}J^{21}P^3+\epsilon_{0312}J^{31}P^2+\epsilon_{0321}J^{32}P^1[/tex]
[tex]= +J^{12}P^3-J^{13}P^2+J^{23}P^1-J^{21}P^3+J^{31}P^2-J^{32}P^1[/tex]
[tex]= (J^{12}P^3+J^{23}P^1+J^{31}P^2)-(J^{13}P^2+J^{21}P^3+J^{32}P^1)[/tex]
and in each parentheses we have an expression identical to the identity I started with.
Therefore, W0 = 0.

likewise I get for all the other W components. So, is W = 0 by definition?

Homework Equations


(none)

The Attempt at a Solution


the only thing I could have missed is the identity from above, but i looks quite solid. I don't see were did I go wrongthanks for your time
tamir
 
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  • #2
You could get to that conclusion faster by noticing that
$$
\epsilon^{\mu\nu\lambda\rho} (x_\nu \partial_\lambda - x_\lambda \partial_\nu) \partial_\rho ~=~ 0 ~,
$$because the partial derivatives commute.

But you're only considering orbital angular momentum, hence it only applies to a spin-0 particle. If there's non-zero intrinsic spin, things are different.

Check Wikipedia's entry on the Pauli--Lubanski vector.
 

FAQ: Is the Pauli-Lubanski Vector Always Zero?

What is the Pauli-Lubanski vector and why is it important?

The Pauli-Lubanski vector is a quantity used in quantum mechanics to describe the intrinsic angular momentum, or spin, of a particle. It is important because it allows us to study the properties of particles at the quantum level and helps us understand the fundamental laws of nature.

Why is the Pauli-Lubanski vector always zero?

The Pauli-Lubanski vector is a combination of the spin and momentum of a particle. In quantum mechanics, the spin and momentum operators do not commute, meaning they cannot be measured simultaneously. This leads to the Pauli-Lubanski vector always being zero, as it is a result of the non-commutativity of these operators.

Can the Pauli-Lubanski vector ever be non-zero?

No, the Pauli-Lubanski vector will always be zero for a single particle. However, in some cases where there are multiple particles, the total spin and momentum can combine to create a non-zero Pauli-Lubanski vector for the system as a whole.

How is the Pauli-Lubanski vector used in particle physics?

The Pauli-Lubanski vector is used in particle physics to classify particles according to their spin and to study their interactions with other particles. It is a fundamental concept in the Standard Model, which is the current theory of particle physics.

Are there any practical applications of the Pauli-Lubanski vector?

While the Pauli-Lubanski vector itself may not have practical applications, the concept of spin has been crucial in the development of technologies such as MRI machines and spintronics, which use the spin of particles to store and process information.

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