Spin Annhilation and Creator Operators Matrix Representation

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The discussion focuses on deriving the matrix representations of the spin raising and lowering operators, S+ and S-, for spin 1/2 particles using the eigenstates of Sz. The user successfully applies the given formula to find that S+ acting on the spin down state yields the spin up state, and vice versa for S-. However, confusion arises regarding how to determine the matrix elements for these operators, as most textbooks skip directly to the matrix forms. Clarification is provided on the notation used in LaTeX, specifically the difference between > and \rangle. The conversation highlights the importance of understanding the transition from state representations to matrix elements in quantum mechanics.
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Homework Statement


Given the expression
s_{\pm}|s,m> = \hbar \sqrt{s(s+1)-m(m\pm 1)}|s,m \pm 1>
obtain the matrix representations of s+/- for spin 1/2 in the usual basis of eigenstates of sz

Homework Equations


s_{\pm}|s,m> = \hbar \sqrt{s(s+1)-m(m\pm 1)}|s,m \pm 1>
S_{+} = \hbar <br /> \begin{bmatrix}<br /> 0 &amp;1 \\<br /> 0 &amp; 0<br /> \end{bmatrix}<br />
S_{-} = \hbar <br /> \begin{bmatrix}<br /> 0 &amp;0 \\<br /> 1 &amp; 0<br /> \end{bmatrix}<br />

The Attempt at a Solution


So I've gotten the first part. You just sub into s and m for spin up or spin down yielding
s_{+}|\downarrow&gt; = \hbar |\uparrow&gt;
s_{-}|\uparrow&gt; = \hbar |\downarrow&gt;
In most textbooks I've checked, they just skip from what I've gotten above straight to the matrix representations. But I'm totally confused as to how the matrix elements of the matrices are found as you go from one to the other.
 
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The matrix element in position ij describes the matrix element between the states i and j, ie,
$$\langle i| A | j\rangle = A_{ij}$$
In your case you only have two states (although the formula given can be used to express the action of ##s_\pm## on a state with higher total spin as well)

Edit: Also note that > is a LaTeX relation whereas \rangle is a LaTeX delimeter. Compare ##|a>## to ##|a\rangle##
 
Orodruin said:
The matrix element in position ij describes the matrix element between the states i and j, ie,
$$\langle i| A | j\rangle = A_{ij}$$
In your case you only have two states (although the formula given can be used to express the action of ##s_\pm## on a state with higher total spin as well)

Edit: Also note that > is a LaTeX relation whereas \rangle is a LaTeX delimeter. Compare ##|a>## to ##|a\rangle##
Thank you so much for explaining. And thanks for the LaTex help. Tried using \ket but that didn't work so had to improvise
 
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