Can anyone prove that the definite integral between minus
infinity and infinity of the Gaussian function is 1?
'Cos I can't.
Love,
GL.
If by the Gaussian function you mean
something like e-x2/2 then here is how:
Consider instead the function e-x2/2 -y2/2 on the x,y-plane.
What is the integral of this over the whole plane? Well you can do
the x and the y integrals separately and get that the answer is the
square of the Gaussian integral you wanted - so if we can do this
new question then we will be able to do the one you wanted.
Okay - the whole function is very rotationally symmetric about the
origin so we should change variables to plane polar coordinates
(r,t). The function becomes e-r2/2 and the area-element dx.dy becomes
r.dr.dt. So we have to integrate:
r.e-r2/2 dr.dt from r=0..infinity
and t=0..2p
Hopefully you will be able to do this integral and you'll see that
the overall integral is 2p.
So the original Gaussian integral had value equal to either
+sqrt(2p) or -sqrt(2p). But it was the integral of an always positive
function and so it must be the former.
AlexB.