How are different potentials implemented experimentally?

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SUMMARY

The discussion focuses on the experimental implementation of various potentials in quantum mechanics, specifically the Dirac-Delta potential, linear potential, and quadratic potential. These potentials, while often artificial, serve as valuable approximations for practical applications in quantum physics. The linear potential is exemplified by its occurrence in circuits with batteries, while the quadratic potential is crucial for understanding harmonic oscillators. Resources for further reading include any standard quantum mechanics textbook that covers these topics extensively.

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  • Understanding of the Schrödinger equation
  • Familiarity with quantum mechanics (QM) concepts
  • Basic knowledge of potential energy functions
  • Experience with experimental physics methodologies
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  • Research the implementation of Dirac-Delta potentials in quantum experiments
  • Study the applications of linear potentials in electrical circuits
  • Explore the role of quadratic potentials in harmonic oscillators
  • Read foundational quantum mechanics textbooks for deeper insights
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Students and professionals in physics, particularly those focused on quantum mechanics, experimental physicists, and educators seeking to enhance their understanding of potential energy applications in quantum systems.

pcflores
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Hi.

I'm wondering how different potentials, such as the Dirac-Delta potential, linear potential, quandratic potenial, etc., are implemented experimentally. I only understand how the Schrödinger equation is solved if these are the potentials and I'd like to have a better understanding of quantum physics by knowing how these are implemented experimentally.

Also, if you guys can suggest some papers or books that I can read, I will really appreciate it.

Thanks!
 
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They generally are not. These are simple potentials offered to get you used to using the Schrödinger equation.

But note: the linear potential is what you get in a wire attached to a battery.
 
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As Simon says: these potentials are artificial. But extremely valuable nevertheless, because they can serve as useful approximations in countless practical cases. The quadratic potential for the harmonic oscillator is a first-order approach for almost any equilibrium situation (##F = -kx##) -- and as such will come back many times throughout any physicist's career. Delta functions mimic 'hard, small things', square wells help understand bound states, and so on.

Any book on QM goes through these potentials, your choice is almost unlimited.
 
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