Solving Delta Potential Barrier Problem with Schrodinger Equation

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Petar Mali
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Homework Statement


In delta potential barrier problem Schrödinger equation we get

[tex]\psi(x)=Ae^{kx}, x<0[/tex]

[tex]\psi(x)=Ae^{-kx}, x>0[/tex]

We must get solution of

[tex]lim_{\epsilon \rightarrow 0} \int^{\epsilon}_{-\epsilon}\frac{d^2\psi}{dx^2}dx[/tex]

Homework Equations


The Attempt at a Solution



[tex]lim_{\epsilon \rightarrow 0} \int^{\epsilon}_{-\epsilon}\frac{d^2\psi}{dx^2}dx=lim_{\epsilon \rightarrow 0} \frac{d\psi}{dx}|^{\epsilon}_{-\epsilon}[/tex] and get the solution

I can say that the whole function is

[tex]\psi(x)=Ae^{-k|x|}[/tex]

I don't have first derivative in 0.

[tex]lim_{\epsilon \rightarrow 0} \int^{\epsilon}_{-\epsilon}\frac{d^2\psi}{dx^2}dx=lim_{\epsilon \rightarrow 0} \int^{0}_{-\epsilon}\frac{d^2\psi}{dx^2}dx+lim_{\epsilon \rightarrow 0} \int^{\epsilon}_{0}\frac{d^2\psi}{dx^2}dx=0[/tex]Why I don't get same solution different then zero like in case

[tex]lim_{\epsilon \rightarrow 0} \int^{\epsilon}_{-\epsilon}\frac{d^2\psi}{dx^2}dx=lim_{\epsilon \rightarrow 0} \frac{d\psi}{dx}|^{\epsilon}_{-\epsilon}[/tex]

?

Homework Statement


Homework Equations


The Attempt at a Solution

 
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First, I'd like to point out how disappointed I was when I clicked on this thread and found that it wasn't a Chuck Norris movie:biggrin:

Petar Mali said:
I can say that the whole function is

[tex]\psi(x)=Ae^{-k|x|}[/tex]

I don't have first derivative in 0.
No you cant. The wavefunction [tex]\psi(x)=\left\{\begin{array}{lr}Ae^{kx}, & x<0 \\ Ae^{-kx}, & x>0\end{array}\right.[/itex] is undefined at [itex]x=0[/itex] (as it should be for a delta function potential). The wavefunction [itex]\psi(x)=Ae^{-k|x|}[/itex] <b>is</b> defined at [itex]x=0[/itex]; the two wavefunctions are not equivalent.<br /> <br /> <blockquote data-attributes="" data-quote="" data-source="" class="bbCodeBlock bbCodeBlock--expandable bbCodeBlock--quote js-expandWatch"> <div class="bbCodeBlock-content"> <div class="bbCodeBlock-expandContent js-expandContent "> [tex]lim_{\epsilon \rightarrow 0} \int^{\epsilon}_{-\epsilon}\frac{d^2\psi}{dx^2}dx=lim_{\epsilon \rightarrow 0} \int^{0}_{-\epsilon}\frac{d^2\psi}{dx^2}dx+lim_{\epsilon \rightarrow 0} \int^{\epsilon}_{0}\frac{d^2\psi}{dx^2}dx=0[/tex]Why I don't get same solution different then zero like in case </div> </div> </blockquote><br /> I don't see how you are getting zero for that limit. Show the rest of your steps.[/tex]
 
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[tex] lim_{\epsilon \rightarrow 0} \int^{\epsilon}_{-\epsilon}\frac{d^2\psi}{dx^2}dx=lim_{\epsilon \rightarrow 0} \int^{0}_{-\epsilon}\frac{d^2\psi}{dx^2}dx+lim_{\epsilon \rightarrow 0} \int^{\epsilon}_{0}\frac{d^2\psi}{dx^2}dx=0[/tex]

[tex]lim_{\epsilon \rightarrow 0} \int^{0}_{-\epsilon}\frac{d^2\psi}{dx^2}dx+lim_{\epsilon \rightarrow 0} \int^{\epsilon}_{0}\frac{d^2\psi}{dx^2}dx=lim_{\epsilon \rightarrow 0}\frac{d\psi}{dx}|^{0}_{-\epsilon}+lim_{\epsilon \rightarrow 0}\frac{d\psi}{dx}|^{\epsilon}_{0}[/tex]

[tex]\frac{d\psi}{dx}=kAe^{kx}[/tex] for [tex]x<0[/tex]

[tex]\frac{d\psi}{dx}=-kAe^{-kx}[/tex] for [tex]x>0[/tex]

[tex]lim_{\epsilon \rightarrow 0} \int^{0}_{-\epsilon}\frac{d^2\psi}{dx^2}dx+lim_{\epsilon \rightarrow 0} \int^{\epsilon}_{0}\frac{d^2\psi}{dx^2}dx=<br /> kA-lim_{\epsilon \rightarrow 0}kAe^{k\epsilon}-lim_{\epsilon \rightarrow 0}kAe^{-k\epsilon}+kA=2kA-2kA=0[/tex]
 
Double check your exponentials (hint hint) and maybe expand them out ignoring terms higher than [itex]\epsilon^1[/itex]