How Do You Construct and Analyze Spin Matrices for a Spin 1 Particle?

In summary: S_x|-1\rangle=(1-0)\frac{\hbar}{2}\sqrt{1(1-1)+1\cdot-1}=-\sqrt{2}\frac{\hbar}{2}Sx=\left(\begin{array}{ccc} \langle 1+0|S_x|0\rangle & \langle 1-0|S_x|-1\rangle \\ \langle 0|S_x|0\rangle & \langle 0|S_x|-1\rangle & \langle 1+0|S_x|+1\rangle
  • #1
mtmcavoy
2
0

Homework Statement


Construct the spin matrices (Sx,Sy,Sz) for a particle of spin 1. Determine the action of Sz, S+, and S- on each of these states.

Homework Equations


s=1 m=-1, 0, 1
Sz=hm |sm>
S+= h [2-m(m+1)]^1/2 |s m+1>
S-= h [2-m(m-1)]^1/2 |s m-1>
*"h" is actually h-bar

The Attempt at a Solution


I've been trying to follow the same method as for spin 1/2, where |1/2 1/2> is a vector (1 0) and |1/2 -1/2> is (0 1), but I don't understand how going between notation for vectors yields these results, and thus I don't know how to get the vector components for the spin 1 case.
 
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  • #2
Use the following equations to construct the matrix:

[tex]
\langle m'|S_x|m\rangle=(\delta_{m,m'+1}+\delta_{m+1,m'})\frac{\hbar}{2}\sqrt{s(s+1)-m'm}
[/tex]

[tex]
\langle m'|S_y|m\rangle=(\delta_{m,m'+1}-\delta_{m+1,m'})\frac{\hbar}{2i}\sqrt{s(s+1)-m'm}
[/tex]

[tex]
\langle m'|S_z|m\rangle=\delta_{mm'}m\hbar
[/tex]

with [itex]s=1[/itex], you know that [itex]m=-1,0,1[/itex].
 
  • #3
Eh, maybe I'm a little more confused than I thought. Can you be a little more...descriptive, maybe? I'm not seeing how those equations apply.
 
  • #4
The spin matrices--for spin 1--look like this:

[tex]
\hat{S}_x=\left(\begin{array}{ccc} \langle 1|S_x|1\rangle & \langle 1|S_x|0\rangle & \langle 1|S_x|-1\rangle \\ \langle 0|S_x|1\rangle & \langle 0|S_x|0\rangle & \langle 0|S_x|-1\rangle \\ \langle -1|S_x|1\rangle & \langle -1|S_x|0\rangle & \langle -1|S_x|-1\rangle
\end{array}\right)
[/tex]

so each 1,0 and -1 are the [itex]m[/itex] and [itex]m'[/itex] values. The delta's are the Kronecker delta:

[tex]
\delta_{mn}= \left< \begin{array}{ll} 1 & m=n \\ 0 & m\neq n\end{array}\right.
[/tex]

It should just be matching the m's and delta's to get values for each component.

EDIT: For a quick example:

[tex]
\langle 1|S_x|0\rangle=(1+0)\frac{\hbar}{2}\sqrt{1(1+1)-1\cdot0}=\sqrt{2}\frac{\hbar}{2}
[/tex]
 

FAQ: How Do You Construct and Analyze Spin Matrices for a Spin 1 Particle?

What are spin matrices for spin 1 and what do they represent?

Spin matrices for spin 1 are mathematical matrices used to describe the intrinsic angular momentum of particles with spin 1. They represent the possible spin orientations of these particles in a given direction.

How do spin matrices for spin 1 differ from spin matrices for other spin values?

Spin matrices for spin 1 differ from those for other spin values in terms of their size and structure. Spin matrices for spin 1 are 3x3 matrices, while those for other spin values can be larger or smaller. Additionally, the elements in spin matrices for spin 1 are all complex numbers, while those for other spin values may also contain real numbers.

How are spin matrices for spin 1 related to the Pauli matrices?

Spin matrices for spin 1 are related to the Pauli matrices through the use of the Gell-Mann matrices. The Gell-Mann matrices are a generalization of the Pauli matrices and are used to describe particles with spin greater than 1/2. The first three Gell-Mann matrices are equivalent to the Pauli matrices, and the remaining six can be used to construct spin matrices for spin 1.

Why are spin matrices for spin 1 important in quantum mechanics?

Spin matrices for spin 1 are important in quantum mechanics because they are used to describe the spin states of particles with spin 1. These spin states are essential for understanding the behavior and properties of these particles, and are crucial in many quantum mechanical equations and calculations.

Can spin matrices for spin 1 be used to calculate the spin of a particle?

No, spin matrices for spin 1 cannot be used to calculate the spin of a particle. They are used to describe the possible spin states of a particle, but the actual spin value must be measured experimentally. The eigenvalues of the spin matrices can provide information about the possible spin values, but they do not determine the actual spin of a particle.

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