HELP ME! Wave Packet equation
The superposition is called a wave packet, and it takes the form: \[\psi (x,t) = \int\limits_{-\infty}^{\infty} dk. A(k)e^{i(kx- \omega t)}\] we begin by considering the wave packet at time t=0 \[\psi (x,0) = \int\limits\limits_{-\infty}^{\infty} dk. A(k)e^{ikx} \] and ilustrate it by considering a special form, called the gaussian form \[A(k) = e^{-\alpha (k-k_{o})^{2}/2}\] proof that: \[\psi (x,0) = \sqrt{\frac{ 2 \pi }{ \alpha }} e^{ik_{o}x} e^{-x^{2}/2\alpha} \]
Well, this would suit better in a mathematical question. Anyways, as physics is mixed with a lot of maths, this will help you, http://en.wikipedia.org/wiki/Gaussian_integral
May be you have found the answer. But in case you have not, this is my proposition. \[\psi(x,0)=\int dk\ e^{-\alpha(k-k_0)^2/2+ikx}=\int dk\ e^{-\alpha(k^2+k_0^2-2kk_0)/2+ikx}=\\ =\int dk\ e^{\alpha k^2/2+\alpha k_0k+ikx-\alpha k_0^2/2}=\int dk\ e^{\alpha k^2/2+k(\alpha k_0+ix)-\alpha k_0^2/2}\] Apply, \[\int dx\ e^{-ax^2+bx+c}=\sqrt{\frac{\pi}{a}}e^{b^2/(4a)+c}\]And you have, \[\sqrt{\frac{2\alpha}{\pi}}e^{(\alpha k_0+ix)^2/(2\alpha)-\alpha k_0^2/2}= \sqrt{\frac{2\alpha}{\pi}}e^{ixk_0}e^{-\alpha x^2/(2\alpha)}\]
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