Astron. Astrophys. 363, 1155-1165 (2000)
Appendix A: The Gaussian kernel method
Consider a sample of size
n: ( ) of identically
distributed, independent random variables. We intend to provide an
estimate of the probability density function of the generic variable
X, namely , defined by the
property:
![[EQUATION]](img391.gif)
If we estimate the probability density function through the
derivative of the empirical repartition function, we obtain a sum of
Dirac functions.
However, if we convolute these Dirac functions by a kernel
which has `good' properties, the
function obtained is then a continuous function and an estimator of
the probability density function (Devroye 1986). The estimator of the
density function of the sample is
denoted , and is given, after
convolution, by:
![[EQUATION]](img394.gif)
where is a parameter which is
fixed with the choice of the kernel applied. This parameter is used to
smooth the shape of the curve, so that
has to tend to zero when n
goes to infinity, but not too fast:
![[EQUATION]](img396.gif)
The `good' properties of
are:
![[EQUATION]](img397.gif)
which ensure the convergence of
in probability to the true density function
of the random variable X.
Therefore:
![[EQUATION]](img399.gif)
A useful kernel is the Gaussian kernel which, moreover, has the
property to be :
![[EQUATION]](img401.gif)
where , and
is the standard deviation.
In our case, , and
.
© European Southern Observatory (ESO) 2000
Online publication: December 5, 2000
helpdesk.link@springer.de  |