QM: Ground State Wave Function of Infinite Square Well

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SUMMARY

The ground state wave function of a particle in an infinite square well is allowed despite appearing to be non-smooth at the boundaries. The key lies in the nature of the potential; when the potential is infinite, the second derivative of the wave function can also be infinite, resulting in a discontinuous first derivative. This behavior is acceptable within the framework of quantum mechanics, particularly when analyzing the time-independent Schrödinger equation. The infinite square well serves as a useful approximation for educational purposes, while finite square wells provide smoother solutions.

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  • Understanding of the time-independent Schrödinger equation
  • Familiarity with wave functions in quantum mechanics
  • Knowledge of potential energy concepts in quantum systems
  • Basic grasp of mathematical continuity and differentiability
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  • Study the implications of infinite potential wells in quantum mechanics
  • Explore the differences between infinite and finite square wells
  • Learn about the mathematical properties of wave functions
  • Investigate the role of boundary conditions in quantum systems
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Students of quantum mechanics, physics educators, and anyone interested in the mathematical foundations of wave functions and potential energy in quantum systems.

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Homework Statement



I was wondering why is the ground state wave function of a particle in an infinite square well allowed? If you drawn it out on a graph, it is one-half of a full sine wave.

But the conditions for an acceptable wave equation is one that is continuous (yes) and "smooth"(no!). How is the ground state allowed, when it "breaks" at the wells?

Homework Equations





The Attempt at a Solution

 
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The wavefunction only has to be smooth when the potential is finite.

For a non-rigorous justification, take a look at the time-independent Schrödinger equation:
[tex]\frac{1}{2m}\nabla^2\psi = (E - V)\psi[/tex]
If the potential V is infinite, then the second derivative of the wavefunction can also be infinite, which corresponds to a discontinuous first derivative, a.k.a. a non-smooth function.
 
I wouldn't worry about it too much. We know that in the real world that infinite isn't ever applicable, it's really only used for approximations and teaching. The finite square well is nicely smooth and continuous (though the transcendental equations make for a non-analytical solution that wouldn't be such a good introduction to quantum).
 

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