Dynamical absorbers system
The dynamic range of any of the detectors is much more limited than the intensity of the beam. In order to increase the linear dynamic range of the scintillator counter and other detectors, a system of dynamical absorbers has been installed. The linearity of the detector is specially important when making comparisons of the absolute intensity, as it is often the case when using the anomalous scattering effect. Furthermore, when measuring both Bragg diffraction and diffuse scattering in the same scan, the dynamical range of the interesting signal can be many orders of magnitude.
A
special card calculates the detector dead time, and depending of the
experimental value and a range of acceptable values set by the user, the system
change the absorber to increase or decrease the intensity arriving to the
detector. The whole operation is automatic, and the controlling program
calculates the corrected intensity in real time. There are absorbers of
different materials and thickness, in order to cover the whole range of energies
used (2.1 – 35 keV).

The following table helps to choose the appropriate absorber material and thickness:
|
Energy (keV |
Material |
Thickness of the base foil (microns) |
|
5.5-7.5 |
Al |
50 |
|
7.5 - 9.5 |
Al |
100 |
|
9-12 |
Al |
200 |
|
|
|
|
|
8 - 11 |
Mo |
12.5 |
|
10.5 - 14 |
Mo |
25 |
|
13 - 18 |
Mo |
50 |
|
17 - 19.5 |
Mo |
100 |
|
19.5- 20.5 |
(use rather Cu) |
|
|
21 – 28 |
Mo |
25 |
|
27 – 35 |
Mo |
50 |
|
|
|
|
|
14 – 25 |
Cu |
50 |
use
rather Mo than Cu whenever possible
technical description of the absorber system
Some commands
filteron
filteroff
filterwhich
f0
… f15
fn = filter with n units of absorber material
fa
filter automatic
fm
filter manual and maximum (f15)
fw
filterwhich
detcor_cal
card software reset
Cabling Diagram: