Time Evolution of the Gaussian packet

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SUMMARY

The discussion centers on the time evolution of a Gaussian wave packet using the propagator equation. The initial wave packet is defined as \(\psi(x',0) = e^{i p_0 x'/\hbar}\frac{e^{-x'^2/2\Delta^2}}{(\pi\Delta^2)^{1/4}}\). Participants clarify that the propagator \(U\) is the free propagator, allowing for a Gaussian integral to derive the time-evolved wave function \(\psi(x,t)\). Misunderstandings regarding the notation "X" as a cross product are addressed, confirming it represents multiplication.

PREREQUISITES
  • Understanding of quantum mechanics, specifically wave functions and propagators.
  • Familiarity with Gaussian integrals and their applications in quantum mechanics.
  • Knowledge of complex exponentials and their role in wave packet formulation.
  • Basic grasp of mathematical notation used in physics, including integrals and multiplication symbols.
NEXT STEPS
  • Study the derivation of the free propagator in quantum mechanics.
  • Learn about Gaussian integrals and their significance in quantum wave packet evolution.
  • Explore the mathematical techniques for solving integrals involving complex exponentials.
  • Review Shankar's "Principles of Quantum Mechanics" for deeper insights into wave packet dynamics.
USEFUL FOR

Students and researchers in quantum mechanics, particularly those studying wave packet dynamics and the mathematical techniques involved in quantum evolution. This discussion is beneficial for anyone seeking clarity on the use of propagators and Gaussian integrals in quantum physics.

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Homework Statement


Can someone give me a general idea (I do not need and probably will not understand the rigorous mathematics) of how you can use the propagator equation

\psi(x,t) = \int{U(x,t;x',t')\psi(x',t')dx'},

the equation for a Gaussian wave packet,

\psi(x',0)= e^{i p_0 x'/\hbar}\frac{e^-x'^2/2\Delta^2}{(\pi\Delta^2)^{1/4}},

to arrive at the equation \psi(x,t) = [\pi^{1/2}(\Delta+\frac{i +\hbar t}{m\Delta})]^{-1/2} <br /> <br /> exp{\frac{-(x-p_0 t/m)^2}{2\Delta^2(1+i \hbar t/m \Delta^2}} <br /> <br /> X exp[\frac{i p_0}{\hbar}(x - \frac{p_0 t}{2m}) ]

Is this just a really complicated integration method? Is that a cross product or multiplcation? If it is a cross product how does come in? See Shankar 154 for more context.




Homework Equations





The Attempt at a Solution


I really do not know of any integration methods that give a cross product so I don't know. Just a general explanation would be helpfull.
 
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If the propagator "U" is the free propagator then you can actually just write it down explicity and then you just have to do a gaussian integral to get the result. If "U" is the propagator for almost any other system the problem gets hella harder.The "X" is not a "cross product." how could it be a cross product!?... there are no vectors!
 
You're right about the cross-product. Then I have no idea why the author used an X instead of a dot for multiplication. It is actually a free propagator. So that is just the result of the Gaussian integral with the propagator and the initial psi...I see.
 

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