QM - Eigenfunction / Eigenvalue Problem

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SUMMARY

The discussion focuses on solving the eigenfunction and eigenvalue problem for the operator defined as a = x + d/dx. The equation aΨ = λΨ leads to the expression Ψ = e^(-1/2 x² + λx + c), where λ represents the eigenvalue. The normalization condition is crucial for determining the spectrum of allowed eigenvalues, indicating that all real values of λ are permissible in this case. The conversation highlights the importance of normalization in more complex scenarios, such as particles in potential wells, to derive discrete energy eigenvalues.

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  • Understanding of quantum mechanics principles, particularly eigenfunctions and eigenvalues.
  • Familiarity with differential operators and their applications in quantum mechanics.
  • Knowledge of normalization conditions in wavefunctions.
  • Basic calculus, including differentiation and integration techniques.
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  • Study the normalization condition for wavefunctions in quantum mechanics.
  • Explore the concept of discrete energy eigenvalues in potential wells.
  • Learn about the role of differential operators in quantum mechanics.
  • Investigate the mathematical techniques for solving differential equations in quantum systems.
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Students and professionals in quantum mechanics, physicists working on eigenvalue problems, and anyone interested in the mathematical foundations of quantum theory.

danny271828
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Homework Statement



Find the eigenfunctions and eigenvalues for the operator:

a = x + [tex]\frac{d}{dx}[/tex]

2. The attempt at a solution

a = x + [tex]\frac{d}{dx}[/tex]

a[tex]\Psi[/tex] = [tex]\lambda[/tex][tex]\Psi[/tex]

x[tex]\Psi[/tex] + [tex]\frac{d\Psi}{dx}[/tex] = [tex]\lambda[/tex][tex]\Psi[/tex]

x + [tex]\frac{1}{\Psi}[/tex][tex]\frac{d\Psi}{dx}[/tex] = [tex]\lambda[/tex]

x + [tex]\frac{d}{dx}[/tex] ln([tex]\Psi[/tex])= [tex]\lambda[/tex]

[tex]\frac{1}{2}[/tex]x[tex]^{2}[/tex] + ln([tex]\Psi[/tex]) = [tex]\lambda[/tex]x +c

[tex]\Psi[/tex] = e^(-[tex]\frac{1}{2}[/tex]x[tex]^{2}[/tex]+[tex]\lambda[/tex]x+c)

[tex]\Psi[/tex] = e^(-[tex]\frac{1}{2}[/tex]x[tex]^{2}[/tex]+[tex]\lambda[/tex])[tex]\Psi[/tex](0)

Not sure from here... I think I plug into initial equation?

a[tex]\Psi[/tex] = [tex]\lambda[/tex][tex]\Psi[/tex]

substituting and using chain rule I obtain...

x[tex]\Psi[/tex] + ([tex]\lambda[/tex]-x)[tex]\Psi[/tex] = [tex]\lambda[/tex][tex]\Psi[/tex]

so x + ([tex]\lambda[/tex] - x) = [tex]\lambda[/tex]

so [tex]\lambda[/tex] = [tex]\lambda[/tex] nope I guess I don't do that... good check though, so I guess this is the correct way to solve for eigenfunction... Can someone help me with finding [tex]\lambda[/tex]?
 
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Normally, the spectrum of allowed eigenvalues [itex]\lambda[/itex] is obtained from the normalization condition. I.e., there should be a non-zero normalization constant (which you denoted by [itex]\Psi(0)[/itex]) such that the integral of the square of the modulus of the wavefunction over entire space (the total probability of finding the particle) is equal to 1. In your case, this doesn't matter, because the wavefunction is normalizable for all real [itex]\lambda[/itex]. So, all values of [itex]\lambda[/itex] are allowed. However, in more complex cases such as a particle in a potential well - the normalization condition would allow you to find the discrete spectrum of energy eigenvalues.

Eugene.

P.S. Perhaps, it is not a good idea to ask the same question in three different threads.

https://www.physicsforums.com/showthread.php?t=182374
https://www.physicsforums.com/showthread.php?t=182369
 
Thanks Eugene...

Sorry about that... Kind of new to this... I havn't seen a way to delete your own posts... but there probably is one...
 

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