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Other Properties

We also note that the odd symmetry of the Fresnel integrals allows other observations among which are:
$\displaystyle \int_{-u}^0 \cos\left(\frac{\pi}{2}x^2\right)$ $\textstyle =$ $\displaystyle C(u)$ (8)
$\displaystyle \int_{-u}^0 \sin\left(\frac{\pi}{2}x^2\right)$ $\textstyle =$ $\displaystyle S(u)$ (9)
$\displaystyle \int_{-u}^u \cos\left(\frac{\pi}{2}x^2\right)$ $\textstyle =$ $\displaystyle 2C(u)$ (10)
$\displaystyle \int_{-u}^u \sin\left(\frac{\pi}{2}x^2\right)$ $\textstyle =$ $\displaystyle 2S(u)$ (11)
$\displaystyle \int_{-\infty}^\infty \cos\left(\frac{\pi}{2}x^2\right)$ $\textstyle =$ $\displaystyle 1$ (12)
$\displaystyle \int_{-\infty}^\infty \sin\left(\frac{\pi}{2}x^2\right)$ $\textstyle =$ $\displaystyle 1.$ (13)



Aaron S. Master 2002-10-17