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

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Homework Help Overview

The discussion revolves around constructing and analyzing spin matrices for a spin 1 particle, specifically the matrices Sx, Sy, and Sz. Participants are exploring the mathematical framework and equations necessary for this task.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to relate the spin 1 case to the spin 1/2 case but expresses confusion about transitioning between vector notations. Some participants provide equations for constructing the matrices but question their applicability. Others seek clarification on the use of Kronecker delta in the context of these matrices.

Discussion Status

Participants are actively engaging with the mathematical concepts, with some providing equations and examples. However, there is a noted lack of clarity among some members regarding the application of these equations, indicating that further exploration and clarification are needed.

Contextual Notes

Participants are working under the constraints of homework guidelines, which may limit the extent of assistance they can provide to one another. There is an emphasis on understanding the underlying principles rather than simply obtaining answers.

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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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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].
 
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.
 
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<br /> \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]
 

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