Normalizing wavefunction obtained from Lorentzian wave packet

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Homework Statement
1. Consider a wave packet with $$ A(k) = \frac {N}{k^2 + \alpha^2} $$
where ##\alpha## is some positive constant. This is Lorentzian wave packet.

a. Find the form of ##\psi(x) ## (You may have to use your knowledge of contour integrals in Complex analysis)
b. Find normalization N such that $$ \int_{-\infty}^{\infty} dx\left | \psi(x) \right |^2 = 1 $$
Relevant Equations
Wave obtained by superposing waves with different amplitude ##A(k)## depending on k is given by:
$$\psi(x) = \int_{-\infty}^{\infty} A(k)e^{ikx}dk $$
Part a: Using the above equation. I got
$$\psi(x) = \int_{-\infty}^{\infty} \frac{Ne^{ikx}}{k^2 + \alpha^2}dk $$

So basically I needed to solve above integral to get the wave function. To solve it, I used Jordan's Lemma & Cauchy Residue Theorem.
And obtained $$\psi(x) = \frac {N \pi e^{-x\alpha}}{\alpha} $$

For part b, I need to find value of N by solving the equation: $$ \frac {\pi ^2 N^2}{\alpha^2} \int_{-\infty}^{\infty} e^{-2x\alpha} dx = 1 $$
Which I obtained as $$|\psi(x)|^2 = \frac {N^2\pi^2}{\alpha^2} e^{-2x\alpha} $$
Now, this integral is not converging. So either my wavefunction is incorrect or I'm doing something wrong in part b. A friend of mine also got same ##\psi(x) ## due to which I'm really confused as to where could we be going wrong.
 
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I'm not able to understand why it will have two contours and not 1 i.e ##x = -\infty## to ## x=+\infty##. Can you please explain