How to Derive Matrix Representations for Spin Operators?

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SUMMARY

The discussion focuses on deriving matrix representations for spin operators in quantum mechanics, specifically for the operators $\hat{S_+}$, $\hat{S_-}$, $\hat{S_x}$, $\hat{S_y}$, and $\hat{S_z}$. The matrices are expressed in terms of the reduced Planck constant $\hbar$ and are essential for understanding spin-1 systems. The provided matrices illustrate the action of these operators on quantum states, which is crucial for applications in quantum computing and quantum mechanics.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly spin systems.
  • Familiarity with linear algebra and matrix operations.
  • Knowledge of the representation of operators in quantum mechanics.
  • Basic grasp of complex numbers and their manipulation.
NEXT STEPS
  • Study the mathematical framework of quantum mechanics, focusing on spin-1 systems.
  • Explore the implications of spin operators in quantum computing applications.
  • Learn about the role of the Pauli matrices in quantum mechanics.
  • Investigate the use of matrix representations in quantum state transformations.
USEFUL FOR

Students and professionals in quantum mechanics, physicists working with quantum systems, and researchers in quantum computing who require a solid understanding of spin operators and their matrix representations.

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Homework Statement
Find the matrix representation of \hat{S_x}, \hat{S_y}, \hat{S_z} for s = 1 spin one (electroweak Z-boson) in the basis of |sm> eigenstates.
Relevant Equations
Hint: do it for \hat{S_\pm} first.
Screen Shot 2020-04-02 at 8.51.02 PM.png

$$\hat{S_+} = \hbar \begin{bmatrix} 0 & \sqrt{2} & 0 \\ 0 & 0 & \sqrt{2} \\ 0 & 0 & 0 \end{bmatrix}$$
$$\hat{S_-} = \hbar \begin{bmatrix} 0 & 0 & 0 \\ \sqrt{2} & 0 & 0 \\ 0 & \sqrt{2} & 0 \end{bmatrix}$$
$$\hat{S_x} = \hbar/\sqrt{2} \begin{bmatrix} 0 & 1 & 0 \\ 1 & 0 & 1 \\ 0 & 1 & 0 \end{bmatrix}$$
$$\hat{S_y} = \hbar/\sqrt{2} \begin{bmatrix} 0 & -i & 0 \\ i & 0 & -i \\ 0 & i & 0 \end{bmatrix}$$
$$\hat{S_z} = \hbar \begin{bmatrix} 1 & 0 & 0 \\ 0 & 0 & 0 \\ 0 & 0 & -1 \end{bmatrix}$$
 
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