How Do You Write the Hamiltonian in the Basis |\theta>?

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SUMMARY

The Hamiltonian for a quantum system is expressed as H = (2e²/ħ²C)−p² - (ħ/2e)I_c cos(−θ), where [−θ, −p] = iħ. To convert this expression into the basis |θ>, one must treat the momentum operator as −iħ∂/∂θ. The final form of the Hamiltonian in the basis |θ> is H = (2e²/C)(∂²/∂θ²) - (ħ/2e)I_c cos(θ). The Laplace operator in spherical polar coordinates is essential for further calculations.

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  • Understanding of quantum mechanics and Hamiltonians
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  • Knowledge of spherical polar coordinates and the Laplace operator
  • Proficiency in calculus, particularly partial derivatives
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TeddyYeo
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Homework Statement



H = \frac{2e^2}{\hbar^2 C} \hat{p^2} - \frac{\hbar}{2e} I_c cos\hat\theta,
where [\hat\theta , \hat{p}] = i \hbar
How can we write the expression for the Hamiltonian in the basis |\theta>

Homework Equations

The Attempt at a Solution



I have already solved most part of the question and this is just one part of it that I am not sure how to convert into the basis form.
Is it that I just now need treat
\hat{p}] = -i \hbar ∇ which is means that it is -i \hbar frac{\partial }{ \partial \theta}
and put
H = \frac{2e^2}{C} \frac{\partial^2}{\partial\theta^2} - \frac{\hbar}{2e} I_c cos\hat\theta
then this is the final form??
 
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Thanks for the post! Sorry you aren't generating responses at the moment. Do you have any further information, come to any new conclusions or is it possible to reword the post?
 
TeddyYeo said:

Homework Statement



H = \frac{2e^2}{\hbar^2 C} \hat{p^2} - \frac{\hbar}{2e} I_c cos\hat\theta,
where [\hat\theta , \hat{p}] = i \hbar
How can we write the expression for the Hamiltonian in the basis |\theta>

Homework Equations

The Attempt at a Solution



I have already solved most part of the question and this is just one part of it that I am not sure how to convert into the basis form.
Is it that I just now need treat
\hat{p}] = -i \hbar ∇ which is means that it is -i \hbar frac{\partial }{ \partial \theta}
No. ##\hat{p^2}=-i \hbar ∇(-i \hbar ∇) =-h^2 \Delta##. Use the Laplace operator written in spherical polar coordinates.
 

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