Wave Function: Normalization Constant

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teme92
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Homework Statement


Consider a free particle, initially with a well defined momentum ##p_0##, whose wave function is well approximated by a plane wave. At ##t=0##, the particle is localized in a region ##-\frac{a}{2}\leq x \leq\frac{a}{2}##, so that its wave function is

##\psi(x)=\begin{cases} Ae^{-ip_0x/\hbar} & if -\frac{a}{2}\leq x \leq\frac{a}{2} \\0 & \text{otherwise} \end{cases}##

Find the normalization constant ##A## and sketch ##Re(\psi(x))##, ##Im(\psi(x))## and ##|\psi(x)|^2##.

Homework Equations

The Attempt at a Solution


So here's what I done:

##A^2\int_{-\frac{a}{2}}^\frac{a}{2} e^{-ip_0x/\hbar}dx=1##

##A^2.-\frac{\hbar}{ip_0}.e^{-ip_0x/\hbar}=1##

##A^2=-\frac{ip_0}{\hbar}.\frac{1}{e^{-ip_0a/2\hbar}-e^{-ip_0a/2\hbar}}##

Is this the correct method? Also I have no idea how to sketch the function asked. Any help would be greatly appreciated.
 
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I took it from ##P(t)=\int_{-\frac{a}{2}}^\frac{a}{2}|\psi(x,t)|^2=1## subbed my wave function into that then. Is this method wrong?
 
##|\psi(x)|^2=A^2e^{-2ip_0z/\hbar}##?
 
No, ##|Z|^2## is the modulus squared ie. ##(\sqrt{a^2+b^2})^2##
 
Is it ##cos\theta +isin\theta##?
 
teme92 said:
##sin2\theta + 1##?

No. You're making this more difficult than it actually is. Forget about a and b and theta. Can you express ##\left| Z \right|^2## in terms of ##Z## and the complex conjugate of ##Z##?
 
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Remember, also. The complex conjugate of ##\psi##, and ##|\psi|^2=\psi^{*}\psi##.

Chris
 
Oh ##|\psi|^2=z\bar{z}##
 
Is it ##\bar{z}=e^{-i\theta}##?
 
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Sorry I was supposed to put a minus in that I'll edit
 
They ##i\theta## and ##-i\theta## cancel each other out so ##e^0=1##
 
So ##|\psi(x)|^2 = 1##?
 
##A=\frac{1}{e^{-ip_0x/\hbar}}##?
 
##A^2\int_{-\frac{a}{2}}^\frac{a}{2} e^{-2ip_0x/\hbar}dx=1##

##A^2.-\frac{\hbar}{ip_0}.e^{-i2p_0x/\hbar}=1##

##A^2=-\frac{ip_0}{\hbar}.\frac{1}{e^{-ip_0a/\hbar}-e^{-ip_0a/\hbar}}##

Is this correct and if so where do I go. Square rooting this seems wrong
 
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I'm getting confused over what ##(Ae^{-i{p_0}x/\hbar})^2## is. And then the integrating of that.