A one-dimensional Gaussian Wave Packet

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SUMMARY

The discussion centers on the integration of a one-dimensional Gaussian wave packet represented by the function \(\varphi_{G}(z,t)\). The integration process involves completing the square and results in the expression \(\exp{\left(-\frac{\Delta k_0^2}{16}(z-ct)^2 + ik_0 (z-ct)\right)}\). The user seeks confirmation of the correctness of their result and assistance in determining the phase and group velocity, as well as identifying any dispersion present in the wave packet.

PREREQUISITES
  • Understanding of Gaussian functions and their properties
  • Familiarity with wave mechanics and the concept of wave packets
  • Knowledge of complex exponentials and integration techniques
  • Basic grasp of phase and group velocity in wave phenomena
NEXT STEPS
  • Study the derivation of phase velocity and group velocity in wave packets
  • Explore the concept of dispersion in wave mechanics and its implications
  • Learn about the method of completing the square in integration
  • Investigate alternative methods for solving integrals involving Gaussian functions
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Students and researchers in physics, particularly those focusing on wave mechanics, quantum mechanics, or applied mathematics, will benefit from this discussion.

Anden
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Homework Statement


I have been given the function
<br /> \varphi_{G}(z,t) = \frac{2}{\Delta k_0\sqrt{\pi}} \int_{-\infty}^{\infty}dk\ e^{-\frac{4(k-k_0)^2}{\Delta k_0^2}}e^{i(kz-\omega t)}<br />
and been told to do the integration and then to specify the phase and group velocity of the wave package. I also have to decide if there is dispersion or not.

Homework Equations


<br /> \omega = ck <br />
<br /> \int_{-\infty}^{\infty}dx e^{-ax^2} = \sqrt{\frac{\pi}{a}},\quad a &gt; 0<br />

The Attempt at a Solution


Using the method of completing the square I get
<br /> \begin{align*}<br /> \varphi_{G}(z,t) <br /> &amp;= \frac{2}{\Delta k_0\sqrt{\pi}} \int_{-\infty}^{\infty}dk\ \exp{\left(-\frac{4(k-k_{0})^2}{\Delta k_{0}^{2}} + i(kz - kct)\right)} \\<br /> &amp;= \frac{2}{\Delta k_0\sqrt{\pi}} \int_{-\infty}^{\infty}dk\ \exp{\left(-\frac{4}{\Delta k_{0}^{2}}(k^2 - 2k(k_0 + i\frac{\Delta k_{0}^{2}}{8}(z-ct)) + k_{0}^{2})\right)} \\<br /> &amp;= \frac{2}{\Delta k_0\sqrt{\pi}} \int_{-\infty}^{\infty}dk\ \exp{\left(-\frac{4}{\Delta k_0^2}( (k-(k_0 + i\frac{\Delta k_0^2}{8}(z-ct)))^2 - 2k_0 i\frac{\Delta k_0^2}{8}(z-ct) + \frac{\Delta k_0^4}{64}(z-ct)^2)\right)} \\<br /> &amp;= \frac{2}{\Delta k_0\sqrt{\pi}} \exp{\left(ik_0(z-ct) - \frac{\Delta k_0}{16}(z-ct)^2\right)} \int_{-\infty}^{\infty}dk\ \exp{\left(-\frac{4}{\Delta k_0^2}(k-(k_0 + i\frac{\Delta k_0^2}{8}(z-ct)))^2\right)} \\<br /> &amp;= \frac{2}{\Delta k_0\sqrt{\pi}} \exp{\left(ik_0(z-ct) - \frac{\Delta k_0}{16}(z-ct)^2\right)} \frac{\sqrt{\pi}\Delta k_0}{2} \\<br /> &amp;= \exp{\left(-\frac{\Delta k_0^2}{16}(z-ct)^2 + ik_0 (z-ct)\right)}<br /> \end{align*}<br />

Now, I don't really have a lot of experience doing things like this (in fact this is the first time). Is the result I got correct or have I done an error somewhere? Also, is there maybe an easier way to calculate the integral?
 
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Finally, I would be grateful if someone could help me with the other parts of the problem, i.e. determining the phase and group velocity, and deciding if there is dispersion or not.
 

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