How Do You Compute the Complex Gaussian Integral I = ∫ e^(-ax^2 + ibx) dx?

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SUMMARY

The integral I = ∫ e^(-ax^2 + ibx) dx, where a > 0 and b are real, can be computed using contour integration techniques. By completing the square in the exponent, the integral simplifies to I = e^(-b^2/4a) ∫ e^(-a(x - ib/2a)^2) dx. The final result is I = (1/√a)e^(-b^2/4a)√π, confirming that the integral converges to this expression as the limits approach infinity.

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homer
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Homework Statement


Let a,b be real with a > 0. Compute the integral
<br /> I = \int_{-\infty}^{\infty} e^{-ax^2 + ibx}\,dx.<br />

Homework Equations


Equation (1):
\int_{-\infty}^{\infty} e^{-x^2}\,dx = \sqrt{\pi}

Equation (2):
-ax^2 + ibx = -a\Big(x - \frac{ib}{2a}\Big)^2 - \frac{b^2}{4a}

The Attempt at a Solution


Completing the square in -ax^2 + ibx gives me Equation (2), so that my integral is now
<br /> I = e^{-b^2/4a}\int_{-\infty}^{\infty} e^{-a(x-ib/2a)^2}\,dx.<br />
Making the substitution u = \sqrt{a}(x-ib/2a) I get du = \sqrt{a}\,dx so tht my integral becomes
<br /> I = \frac{1}{\sqrt{a}}\,e^{-b^2/4a}\int_{-\infty - ib/2\sqrt{a}}^{\infty - ib/2\sqrt{a}} e^{-u^2}\,du.<br />

But this doesn't seem right.
 
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You've got it right. Just note that ##-\infty - ib/2\sqrt{a}=-\infty## and ##\infty - ib/2\sqrt{a}=\infty##, and you're basically done.
 
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Thanks Zeta. Huge brain fart on my part in making it rigorous. The integral I was trying to compute is the limit of

I(R_1, R_2) = \int_{-R_1}^{R_2} e^{-ax^2 + bx}\,dx

as R_1, R_2 \to \infty. Then I can make a subsitution z = \sqrt{a}(x-ib/2a) to get the integral

I(R_1,R_2) = \frac{1}{\sqrt{a}}\,e^{-b^2/4a}\int_{-\sqrt{a}R_1-ib/2\sqrt{a}}^{\sqrt{a}R_2 - ib/2\sqrt{a}}e^{-z^2}\,dz.

The integrand e^{-z^2} is analytic on the entire complex plane, so the integral is path independent. So in particular I can take it on a contour consisting of:

(1) A straight line up from z = -\sqrt{a}R_1 - ib/\sqrt{a} up to the real axis at point z = -\sqrt{a}R_1.

(2) A straight line on the real axis from z = -\sqrt{a}R_1 to z = \sqrt{a}R_2.

(3) A straight line down from the real axis at point z = \sqrt{a}R_2 to z = \sqrt{a}R_2 - ib/2\sqrt{a}.

Taking the limit as R_1, R_2 \to \infty the integrals on contour sections (1) and (3) vanish since \lvert z\rvert \to \infty and thus e^{-z^2} \to 0 on these two vertical lines. The integral on contour (2) then becomes

\lim_{R_1, R_2 \to \infty}\int_2 e^{-z^2}\,dz = \int_{-\infty}^{\infty} e^{-x^2}\,dx = \sqrt{\pi}.

Thus we have

\begin{align*}
\int_{-\infty}^{\infty} e^{-ax^2 + bx}\,dx
& = \lim_{R_1,R_2 \to \infty} I(R_1,R_2) \\
& =
\lim_{R_1,R_2 \to \infty} \frac{1}{\sqrt{a}}\,e^{-b^2/4a}\int_{-\sqrt{a}R_1-ib/2\sqrt{a}}^{\sqrt{a}R_2 - ib/2\sqrt{a}}e^{-z^2}\,dz \\
& = \frac{1}{\sqrt{a}}\,e^{-b^2/4a}\sqrt{\pi}.
\end{align*}
 
Oops, contour (1) should be from z = -\sqrt{a}R_1 - ib/2\sqrt{a} to z = -\sqrt{a}R_1.
 

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