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

AI Thread Summary
The discussion focuses on computing the complex Gaussian integral I = ∫ e^(-ax^2 + ibx) dx, where a and b are real numbers with a > 0. The integral is transformed by completing the square, leading to the expression I = e^(-b^2/4a) ∫ e^(-a(x - ib/2a)^2) dx. A substitution is made to simplify the integral, and it is noted that the limits of integration can be extended to infinity without affecting the result due to the properties of the integrand. The final result is derived as I = (1/√a)e^(-b^2/4a)√π, confirming the correctness of the approach. The discussion emphasizes the importance of contour integration and the behavior of the integrand at infinity.
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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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