How Do You Determine the Width of a Gaussian Wavepacket in Real Space Over Time?

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Hi, this type of question has been confusing my slightly as of late, an a pointer in the right direction would be greatly appreciated

Homework Statement


The wavefunction associated with a Gaussian wavepacket propagating in free space can be shown to be [included as attachment - it's too complicated for here] where delta k is withe width of the wavepacket in k space and v is the velocity of the wavepacket.

Deduce an expression for the width of the wavepacket in real space (z-space)as a function of time


Homework Equations



again, as attached

The Attempt at a Solution



I'm suspecting it has something to do with Fourier Transforms, but I'm really stumped. it's probably straightforward, but I'm a bit blind to it at the moment

Thanks in advance
 
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I have a hunch that [itex]\Delta z\Delta p =\frac{\hbar}{2}[/itex], since a gaussian wavepacket is minimizing the uncertainty relations.

Daniel.
 
To find the witdth of the wave packet you should consider the form of
[tex]|\psi|^2[/tex] .
This will have the form
[tex]\psi \propto \exp \left\{- \frac{(z - vt)^2}{A(t)} \right\}[/tex]

This has the form of a Gaussian curve. The maximum occurs where [tex]z = vt[/tex] where the exponens takes on the value 1.
The width is given by the length between the points where the exponent is [tex]1/2[/tex]. So the expression used to find the widht is
[tex]\exp \left\{ - \frac{(z-vt)^2}{A(t)} \right\} = \frac{1}{2}[/tex].
Solving this gives two solutions [tex]z_1(t)[/tex] and [tex]z_2 (t)[/tex] and the difference between these are the width of the wave packet.

You can expect that the width is increasing with time, since the Schrödinger equation has a dispersive term (a term that causes different Fourier components of the wave to propagate with different velocities).
 
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