Wave function in terms of Basis Functions

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Homework Help Overview

The discussion revolves around expressing the function g(x) = x(x-a) e^{ikx} in terms of a series of basis functions, specifically the sine functions defined for a particle in a box scenario. Participants are exploring the implications of the function's domain and its representation in the context of quantum mechanics.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants are considering the appropriate domain for g(x) and whether it should be limited to the interval from 0 to a. There is discussion about finding the expansion coefficients using principles of orthogonality related to Fourier series. Some participants express uncertainty regarding the application of these principles to the given function.

Discussion Status

The discussion is ongoing, with participants sharing insights about the completeness of the basis functions and the potential methods for determining the expansion coefficients. There is a recognition of the need to clarify the function's domain and the application of Fourier's theorem, but no consensus has been reached yet.

Contextual Notes

Participants are operating under the assumption that the function models a particle in a box, which imposes specific constraints on the problem setup. The discussion reflects varying levels of confidence regarding the application of Fourier series and the properties of the eigenfunctions involved.

Domnu
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Problem
We have the function [tex]g(x)=x(x-a) \cdot e^{ikx}[/tex]. Express [tex]g(x)[/tex] in the form

[tex]\sum_{n=1}^\infty a_n \psi_n (x)[/tex]

where

[tex]\psi_n = \sqrt{\frac{2}{a}} \sin \(\frac{n\pi x}{a}\)[/tex]

Solution
I have absolutely no clue as to how to start... I know a bit about Fourier series, but here, the function [tex]g(x)[/tex] has an infinite period.
 
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Actually wait... we can just let [tex]g(x)[/tex] go from 0 to a, since it's supposed to model a particle in a box from potential walls 0 to a.
 
my guess would be that you could do it from 0 to a. So, I believe the problem now is to find the expansion coefficients An. To do this you will have to use Fourier's principle of orthogonality. I'm not 100 percent sure though, but it seems reasonable.
 
The set [itex]\{\psi_{n}(x)\}[/itex] is complete, which means you can express any (well behaved, piecewise continuous) function as a linear combination of its elements. The coefficients which act as weights are to be determined by Fourier's theorem.

These are actually eigenfunctions for a particle in a 1D box. Eigenfunctions are complete by definition.
 

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