A particle with spin 1/2 in a potential well

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SUMMARY

The discussion focuses on finding the energy levels of a spin 1/2 particle in a potential well defined by the equation V(r) + W(r)*(l,s), where V(ra) = 0, and W(r) = q*δ(r-a). Participants emphasize the necessity of solving the radial Schrödinger equation without the (l,s) term, which simplifies the problem. The interaction of the angular momentum and spin in the delta layer is addressed through the vector product equation, leading to a transformation of the stitching condition for wave functions at the boundary.

PREREQUISITES
  • Understanding of the radial Schrödinger equation
  • Familiarity with quantum mechanics concepts such as spin and angular momentum
  • Knowledge of delta functions in potential wells
  • Proficiency in LaTeX for formatting equations
NEXT STEPS
  • Study the radial Schrödinger equation in detail
  • Explore the implications of spin 1/2 particles in quantum mechanics
  • Learn about delta potentials and their applications in quantum systems
  • Review the use of LaTeX for presenting mathematical equations effectively
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Students and researchers in quantum mechanics, particularly those focusing on potential wells and spin interactions, as well as educators seeking to enhance their understanding of advanced physics problems.

kisdrA
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Hello everyone. Help me solve the problem. I don't understand how to handle this type of task.

Find the energy levels of a spin 1/2 particle in a potential well: V(r)+W(r)*(l,s), where V(r<a)=-U, V(r>a)=0, W(r) = q*δ(r-a)
 
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Moderator's note: Thread moved to advanced physics homework help.

@kisdrA you will need to post any relevant equations and show your attempt at a solution.
 
1734856353093.png
 
It is clear that the problem in the potential ##V(r)+W(r)*(l,s)##, but without the (l,s) term: ##V(r)+W(r)##, simply reduces to solving the radial Schrödinger equation. And I understand how to find energy levels in such a task. But what to do when ls interaction also appears in the delta layer?
 
A vector product can be written like this.
##(\overrightarrow{l}, \overrightarrow{s}) = \frac{1}{2} (\overrightarrow{j}^2 - \overrightarrow{l}^2 - \overrightarrow{s}^2)##
Then maybe just transform the stitching condition?
##\Psi^{'}_{II}(a+0) -\Psi^{'}_{I}(a-0) = \frac{2m}{\hbar^{2}}*q*\frac{1}{2}(j(j+1)-l(l+1)-s(s+1)) \Psi_{I,II}(a\pm 0)##
 
kisdrA said:
@kisdrA posting text and equations in images is not allowed here. Please post text and equations directly; use the PF LaTeX feature for equations. There is a LaTeX Guide link at the bottom left of each post window.
 

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