Spin Annhilation and Creator Operators Matrix Representation

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SUMMARY

The discussion focuses on obtaining the matrix representations of the spin raising and lowering operators, \( S_{+} \) and \( S_{-} \), for spin-1/2 systems. The expressions derived are \( S_{+} = \hbar \begin{bmatrix} 0 & 1 \\ 0 & 0 \end{bmatrix} \) and \( S_{-} = \hbar \begin{bmatrix} 0 & 0 \\ 1 & 0 \end{bmatrix} \). The participants clarify the process of transitioning from the action of these operators on the spin states to their matrix representations, emphasizing the significance of matrix elements in quantum mechanics. Additionally, they address common LaTeX formatting issues encountered while discussing these concepts.

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  • Understanding of quantum mechanics, specifically spin-1/2 systems
  • Familiarity with the notation and operations of raising and lowering operators
  • Knowledge of matrix representation in quantum mechanics
  • Proficiency in LaTeX for formatting mathematical expressions
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  • Learn about the implications of spin operators in quantum mechanics
  • Explore the use of LaTeX for advanced mathematical formatting
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Students and professionals in quantum mechanics, physicists working with spin systems, and anyone interested in the mathematical representation of quantum operators.

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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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