As suggested in the comment, write the integral as
$$\Re\int_0^{\infty} dx \, e^{-(1-i) x^2} = \Re\int_0^{\infty} dx \, e^{-\sqrt{2} e^{-i \pi/4} x^2}$$
Now consider the following contour integral:
$$\oint_C dz \, e^{-\sqrt{2} e^{-i \pi/4} z^2}$$
where $C$ is a circular sector of radius $R$ that opens at an angle of $\pi/8$ with respect to the positive real axis. Note that we will not be using residues in computing the integral, because there are no poles within the contour $C$. Rather, we will be evaluating the integral over the contour itself and using Cauchy's theorem.
The contour integral over $C$ is equal to
$$\int_0^R dx \, e^{-\sqrt{2} e^{-i \pi/4} x^2} + i R \int_0^{\pi/8} d\theta \, e^{i \theta} \, \exp{\left[-\sqrt{2} R^2 e^{-i \pi/4 + 2 \theta}\right]}\\+e^{i \pi/8} \int_R^0 dt \,e^{-\sqrt{2} t^2} $$
Note that the second integral vanishes as $R \to \infty$. Its magnitude is bounded by
$$R \int_0^{\pi/8} d\theta \, e^{-\sqrt{2} R^2 \sin{(\pi/4+2 \theta)}} \le R \int_0^{\pi/8} d\theta \, e^{-\sqrt{2} R^2/2} e^{-4 \sqrt{2} R^2 \theta/\pi} \le \frac{\pi}{4 \sqrt{2} R} e^{-\sqrt{2} R^2/2}$$
as $R \to \infty$. Further, the contour integral is zero by Cauchy's theorem (no poles in the contour). Therefore,
$$\int_0^{\infty} dx \, e^{-(1-i) x^2} = e^{i \pi/8} \int_0^{\infty} dt \,e^{-\sqrt{2} t^2} = \frac12 e^{i \pi/8} \sqrt{\frac{\pi}{\sqrt{2}}}$$
Therefore, taking real parts, we get
$$\int_0^{\infty} dx \, e^{-x^2} \cos{x^2} = \frac{\sqrt{\pi}}{2} \frac{\cos{(\pi/8)}}{2^{1/4}} = \frac{\sqrt{\pi}}{4} \sqrt{1+\sqrt{2}}$$