The speckle field generated by a stocastic sample is formed by
speckles extending in both the orthogonal and parallel direction
with respect to the direction of propagation of the wave. The intensity
measured in a plane perpendicular to the direction of propagation
varies as the plane is moved; small movements
of the plane will give small variations in the intensities. As a matter
of facts, the speckles appear and disappear as the plane is moved. This
allows us to speack of the three dimensional appearence of the speckles.
We will show that the speckles are elongated in the direction
of the propagation of the light. If the diamer is
times a wave
length
, their length is
times
.
In the following sections, we will show that the three dimensional correlation function of the intensity of the scattered light gives more informations than the two dimensional one; in some cases it is possible to determine the sign of the field correlation function, thus determining it completely. Moreover, in analogy to the quadratic relation between the diameter and length of a speckle, the longitudinal frequencies should be related to the square root of the frequencies of the sample: measuring the longitudinal correlations should double the dynamic of the system.