Can a Double Integral be Simplified Using a Substitution of Polar Coordinates?

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The discussion focuses on simplifying the double integral \(\int_{0}^{\infty}dx \int_{0}^{\infty}dy e^{i(x^{2}-y^{2})}\) using a substitution of polar coordinates. The proposed substitution involves \(x = r \cosh(u)\) and \(y = r \sinh(u)\), leveraging the identity \(\cosh^2(u) - \sinh^2(u) = 1\). The transformation aims to express the integral in terms of radial and angular components, ultimately leading to the evaluation of the integral as \(2 \int_0^{\infty} \cos x^2 \, dx = \sqrt{\frac{\pi}{2}}\). The discussion highlights the potential for analytic methods alongside coordinate transformations.

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If we wish to calculate the integral.

[tex]\int_{0}^{\infty}dx \int_{0}^{\infty}dy e^{i(x^{2}-y^{2}}[/tex]

which under the symmetry [tex](x,y) \rightarrow (y,x)[/tex] it gives you the complex conjugate counterpart.

my idea is to make the substitution (as an analogy of Laplace method)

[tex]x=rcosh(u)[/tex] , [tex]y=rsinh(u)[/tex] (or viceversa) using the fact that the square of cosh minus square of sinh is equal to one and expressing the integral as:

[tex]\int_{0}^{\infty}dr re^{ir^{2}}d\Omega[/tex]

the integral Omega is over the angle variable u, if we knew tha exact value of Omega the the radial part is just the imaginary number "i" if i am not wrong.
 
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Here is a way do to this without any substitutions.

We can write:
[tex]\int_0^{\infty} e^{-iy^2} \ dy \cdot \int_0^{\infty} e^{ix^2} \ dx[/tex]

Use Euler's formula:
[tex]\left( \int_0^{\infty} \cos y^2 - i\sin y^2 \ dy \right) + \left( \int_0^{\infty} \cos x^2 + i \sin x^2 \ dx \right)[/tex]

Which can be combined into:
[tex]2 \int_0^{\infty} \cos x^2 \ dx = \sqrt{ \frac{\pi}{2}}[/tex]
 
Thanks kummer, i know that the integra proposed can be made by simple analytic method however i would like to know how to perform the integral with my transformation of coordinates, so if we can map the rectangle.

[tex]R= (0, \infty) x(0,\infty)[/tex] Cartesian coordinates

to [tex]V= (0, \infty) x(-\pi,\pi)[/tex] Polar (??) coordinates

[tex]x=r cosh(u)[/tex] and the same for y with the hyperbolic sine.
 

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