Gaussian integral

The Gaussian integral, also known as the Euler–Poisson integral, is the integral of the Gaussian function e−x2 over the entire real line. It is named after the German mathematician Carl Friedrich Gauss. The integral is: Abraham de Moivre originally discovered this type of integral in 1733, while Gauss published the precise integral in 1809. The integral has a wide range of applications. For example, with a slight change of variables it is used to compute the normalizing constant of the normal distribution. The same integral with finite limits is closely related to both the error function and the cumulative distribution function of the normal distribution. In physics this type of integral appears frequently, for example, in quantum mechanics, to find the probability density of the ground state of the harmonic oscillator. This integral is also used in the path integral formulation, to find the propagator of the harmonic oscillator, and in statistical mechanics, to find its partition function. Although no elementary function exists for the error function, as can be proven by the Risch algorithm, the Gaussian integral can be solved analytically through the methods of multivariable calculus. That is, there is no elementary indefinite integral for but the definite integral can be evaluated. The definite integral of an arbitrary Gaussian function is The Gaussian integral is encountered very often in physics and numerous generalizations of the integral are encountered in quantum field theory. A standard way to compute the Gaussian integral, the idea of which goes back to Poisson, is to make use of the property that: Consider the function e−(x2 + y2) = e−r2 on the plane R2, and compute its integral two ways: