How do I effectively normalise the Schrodinger PDF with given conditions?

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Homework Help Overview

The discussion revolves around the normalization of the Schrödinger wave function \(\Psi(x,t) = Ae^{-\lambda |x|}e^{-i \omega t}\). Participants are exploring the conditions required for normalization, specifically ensuring that the integral of the squared modulus of the wave function equals one.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the process of finding the normalization constant \(A\) by integrating the squared modulus of the wave function. Questions arise about the validity of initial steps and the correct application of the complex conjugate in the normalization process.

Discussion Status

Some participants have provided guidance on the importance of using the complex conjugate when calculating \(|\Psi|^2\). There is an ongoing examination of the steps involved in the normalization process, with some participants questioning the correctness of previous calculations and assumptions.

Contextual Notes

Participants are working under the constraints of ensuring that the normalization condition \(\int_{-\infty}^{\infty} |\Psi (x,t)|^2 dx=1\) is satisfied, while also addressing potential errors in earlier calculations.

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Homework Statement



Normalise
[tex]\Psi(x,t) = Ae^{-\lambda |x|}e^{-i \omega t}[/tex]

Homework Equations



(i.e. it must satisfy [tex]\int_{-\infty}^{\infty} |\Psi (x,t)|^2 dx=1[/tex])

The Attempt at a Solution



This is my first attempt at normalisation and I don't know how valid my reasoning is, can someone please check to see if I'm doing it right:

[tex]\int_{-\infty}^{\infty}|\Psi (x,t)|^2 dx = \frac{A^2}{\lambda} e^{-2 i \omega t}[/tex]

[tex]\Rightarrow \frac{\lambda}{A^2}e^{2i \omega t} \int_{-\infty}^{\infty}|\Psi (x,t)|^2 dx =1[/tex]

[tex]\int_{-\infty}^\infty \left(\frac{\sqrt{\lambda}}{A}e^{i\omega t} |\Psi|\right)^2dx =1[/tex]

[tex]\therefore \Psi (x,t)_{normalised} = \frac{\sqrt{\lambda}}{A}e^{i\omega t} \times \left(Ae^{-\lambda |x|}e^{-i \omega t}\right) = \sqrt{\lambda}e^{-\lambda |x|}[/tex]

thanks
 
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First, recall that [itex]|\Psi (x,t)|^2[/itex] means [itex]\Psi^*(x,t) \Psi(x,t)[/itex]. That is, you multiply [itex]\Psi(x,t)[/itex] by its complex conjugate [itex]\Psi^*(x,t)[/itex].

What is the complex conjugate of the [itex]\Psi(x,t)[/itex] that you were given?
 
Oh, right! So I can't just square it?

The conjugate would be [tex]Ae^{-\lambda |x|}e^{i \omega t}[/tex]

So I just times those together to find [tex]|\Psi|^2[/tex]?

Are my other steps sound though (assuming that I fix the start up)?

Thanks again
 
Your other steps will be completely different. For one thing, the e^ part becomes 1 and you won't have to worry about it. You should get a value for A, which makes sense because normalization means finding the amplitude A that goes in front of the wavefunction.
 
Thanks for your help! Is this correct now?

[tex]\begin{array}{cclc}\int_{-\infty}^\infty |\Psi|^2dx &=& 2\int_{0}^\infty (Ae^{-\lambda x}e^{-i \omega t} Ae^{-\lambda x}e^{i \omega t})dx & \ \ \ \ \ \ \ \ \ \int_{-\infty}^\infty f(|x|)dx = 2\int_0^\infty f(x)dx \\\\ &=& 2\int_0^\infty A^2e^{-2\lambda x}dx & \\\\ &=& \dfrac{A^2}{\lambda}& \end{array}[/tex]

so the answer is [tex]A = \sqrt{\lambda}[/tex]?
 
Last edited:
Almost, but e^-λx * e^-λx = e^-2λx.
 
thanks!
 

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