Eigenvalues and Eigenstates of Spin Operator

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SUMMARY

The discussion focuses on finding the eigenvalues and eigenstates of a spin 1/2 particle using the spin operator expressed in arbitrary directions with the Pauli Matrices. The spin operator is defined as n·σ = ℏ/2(cosφsinθσ_x + sinφsinθσ_y + cosθσ_z). The participant successfully solved the eigenvalue equation n·σΨ = λΨ, yielding eigenvalues of ±ℏ/2. They seek more efficient techniques for similar problems, suggesting the use of a rotated coordinate system to simplify calculations.

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  • Understanding of Pauli Matrices and their matrix forms
  • Familiarity with eigenvalue equations in quantum mechanics
  • Knowledge of spin operators and their representations
  • Basic concepts of rotation matrices in quantum mechanics
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  • Learn about rotation matrices and their applications in quantum state transformations
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Quantum mechanics students, physicists working with spin systems, and researchers seeking efficient methods for solving eigenvalue problems in quantum theory.

thepopasmurf
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I'm not exactly looking for help finding the eigenvalues of the spin operator, I'm mainly wondering if there is a better technique to do it.

Homework Statement


Find the eigenvalues and corresponding eigenstates of a spin 1/2 particle in an arbitrary direction (θ,\phi) using the Pauli Matrices

Homework Equations


Spin operator in arbitrary direction:
n.\sigma = \hbar/2(cos\phisin\theta\sigma_x + sin\phisin\theta\sigma_y+cos\theta\sigma_z)

\sigma_x,\sigma_y,\sigma_z/are the Pauli spin matrices.<br /> <br /> <br /> <h2>The Attempt at a Solution</h2><br /> <br /> The way I did it was to express the pauli matrices in their matrix form, sum up the expression to get one matrix, then solve the eigenvalue equation<br /> n.\sigma\Psi = \lambda\Psi.<br /> <br /> This gives me the answer \pm\hbar/2<br /> <br /> My question is: Is there a better/quicker way to do this (and problems similar to this) without having to solve the eigenvalue equation directly? I have other similar questions where solving the eigenvalue equation becomes long and tedious.
 
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What you've done is the "direct" way to solve these problems. There are tricks you can use in special cases, but I'm not sure if it's possible to make it much easier in general. You could use a coordinate system which is rotated such that the z axis lies along the direction \hat{n}, so that the spin operator is just \sigma_z. For this you would have to use the rotation matrix that converts \Psi into the new coordinate system, \exp[i\theta(\sigma_y\cos\phi + \sigma_x\sin\phi)/2] (or something like that).
 

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