What does it mean to find eigen values and functions of an infinite well?

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SUMMARY

The discussion focuses on the significance of finding eigenvalues and eigenfunctions of an infinite potential well in quantum mechanics. When solving the Schrödinger equation for this scenario, the eigenvalues represent the quantized energy levels of a particle, while the eigenfunctions correspond to the wavefunctions associated with these energy states. The wavefunction's magnitude squared indicates the probability density of locating the particle at a specific point. Additionally, particles can exist in states represented by linear combinations of eigenfunctions, leading to a range of possible wavefunctions defined by Fourier series.

PREREQUISITES
  • Understanding of the Schrödinger equation
  • Familiarity with quantum mechanics concepts such as wavefunctions and probability density
  • Knowledge of eigenvalues and eigenfunctions
  • Basic principles of Fourier series
NEXT STEPS
  • Study the solutions to the Schrödinger equation for various potential wells
  • Explore the concept of linear combinations of eigenfunctions in quantum mechanics
  • Learn about the implications of probability density in quantum states
  • Investigate the role of Fourier series in representing wavefunctions
USEFUL FOR

Students and professionals in physics, particularly those specializing in quantum mechanics, as well as educators seeking to explain the concepts of eigenvalues and eigenfunctions in the context of infinite potential wells.

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What does it mean to find eigenvalues and eigen functions of an infinite well?
 
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When you solve the Shrodinger equation for an infinite well potential and obtain the eigenvalues and eigenfunctions you are finding the allowed states of a particle subjected to this potential. The only energies that a particle like this could ever be measured to have are the energy eigenvalues. The eigenfunctions represent the possible wavefunctions of the particle when it has a definite energy. Remember that the interpretation of the wavefunction is that its magnitude squared at a given point gives the probability density for the particle to be located at that point

It is possible for the particle to have wavefunctions other than the eigenfunctions. The particle can have a wavefunction that is any linear combination of the eigenfunctions. In the case of the infinite well potential the eigenfunctions are the sin and cos functions, so the possible wavefunctions are very general: any function with a Fourier series. But, if the particle does not have an eigenfunction as a wavefunction then we can not be sure what energy the particle will be measured to have. The probability that a given eigenvalue of the energy will be measured corresponds to the coefficient of the eigenfunction in the linear combination.
 

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