Incident Beam Part consists of X-ray Tube and Incident
Beam Optics.
To see detailed overview, please click on items listed
on the left.
High Resolution
Incident Beam Optics
Medium Resolution
Incident Beam Optics
X-ray Tube
Ceramic diffraction x-ray tube
Main Properties
Anode Material |
Wavelength Ka1 (Å) |
Wavelength Ka2 (Å) |
Wavelength Ka (Å) |
Cu |
1.54056 |
1.54439 |
1.54184 |
Focus |
Focus Type |
Focus Dimensions |
|
Line |
LFF (Long Fine Focus) |
12 mm X 0.4 mm |
|
Be window diameter |
Be window thickness |
Working Power |
Standby Power |
14 mm |
300 mm |
45 kV / 40 mA |
30 kV / 20 mA |
Beam Attenuators & Filters
Beam attenuator is an absorber which is placed in
the x-ray beam to reduce its intensity by a specific factor.
Specific beam attenuators are designed for use with
x-ray mirrors and hybrid monochromators.
Attenuation Factors for Cu Ka
radiation
Copper foil (0.1 mm) |
Combined Copper (0.2 mm) / Nickel (0.02 mm) |
~ 100 |
~ 10,000 |
Automatic Beam Attenuator contains a Ni foil that
can be set to be switched in and out of the x-ray beam either at
a fixed angle or at a fixed intensity. Operation is controlled by
the Data Collector software.
Automatic Beam Attenuator Operating Modes
Mode |
Application |
Do not switch (Activated/Deactivated) |
Beam attenuator stays either inserted into the x-ray beam
path or removed over a whole angular range and for the full
measuring time. |
At pre-set intensity |
Beam attenuator is inserted into the beam when the specified
count rate ("activate" level) is reached, and/or is
removed from the beam when the count rate drops below another
specified value ("deactivate" level). |
At pre-set angle |
Beam attenuator is inserted into the beam when diffractometer
position on th scan axis is inside the specified interval. The
interval is given by the activate and deactivate angles. |
Beta-filter
Tube Anode |
Beta-filter |
Thickness (mm) |
Kb intensity reduction (%) |
Ka intensity reduction (%) |
Cu |
Ni |
20 |
99 |
58 |
Fixed Divergence Slits
Divergence slits are fitted in the incident beam path
to control the equatorial divergence of the incident beam.
Four fixed divergence slits marked 1/2o,
1/4o, 1/16o,
and 1/32o are used in X'Pert diffractometer.
Fixed divergence slits must be inserted into the slot for fixed divergence
slits on the PreFIX module.
The length of the area on the sample that is irradiated
by the incident beam is dependent on the divergence of the x-ray beam
and the position of the sample with respect to the beam. It can be
calculated as follows:
L - irradiated length of the sample,
R - radius of the goniometer (R = 320mm),
d - divergence angle as is engraved on
the fixed divergence slit,
w - angle between incident beam and the
sample surface.
Incident Beam Masks
Beam masks are fitted in the incident beam path to
control the axial width of the incident beam, defining the amount
(width) of the sample that is irradiated by the incident x-ray beam.
The size of the beam mask opening must be such that
the incident x-ray beam is completely accepted by the sample during
the complete measurement.
The total width of the area on the sample irradiated
by the incident beam is dependent on the size of the x-ray beam and
the position of the sample with respect to the beam.
X-ray Mirror
The graded multilayer parabolic x-ray mirror is a special
kind of beam conditioner, which is able to convert the divergent x-ray
beam from a line focus tube to an intense monochromatic quasi-parallel
beam. X-ray mirror provided with X'Pert diffractometer is designed
to diffract characteristic Ka radiation.
Kb radiations suppressed to a level below
0.5% of its original level.
The x-ray mirror accepts ~0.8o
of the x-ray beam from the line focus of the x-ray tube. The quasi-parallel
beam diffracted by the mirror has a small horizontal (equatorial)
divergence (< 0.05o). The beam from
the x-ray mirror is ~1.2mm high and ~20mm
wide. The beam emitted from the x-ray mirror is offset relative
to the direst beam from the x-ray tube. This offset angle is referred
to as the "mirror offset". The data collector software will
always apply an offset whenever the x-ray mirror is present in the
incident beam path.
Slit size and the irradiated length
Slit Marking |
Beam height (mm) |
Irradiated length (mm) |
1/2o |
1.2 |
0.12 + 1.2 / sin(w) |
1/4o |
0.6 |
0.12 + 0.6 / sin(w) |
1/8o |
0.3 |
0.12 +0.3 / sin(w) |
1/16o |
0.15 |
0.12 + 0.15 / sin(w) |
w - angle between the incident
beam and the sample surface.
Hybrid Monochromator
The hybrid monochromator is a special kind of beam
conditioner, which is able to convert the divergent x-ray beam from
a line tube focus to a quasi-parallel beam with a pure Ka1
radiation component. It consists of a parabolic-shaped multilayer
mirror and a special channel-cut Ge crystal.
Hybrid monochromator will offset the x-ray beam. The
hybrid monochromator passes slightly broader spectral range than traditional
four-crystal monochromator and therefore delivers a much more intense
parallel beam of Ka1 radiation. Ka2
component is suppressed to a level below 0.1%. It may become visible
during reciprocal space mapping with large dynamic range.
X-ray Lab owns hybrid monochromator 4X, consisting
of a combination of an x-ray mirror and a 2-crystal Ge(220) 4-bounce
monochromator. The acceptance angle from line focus of the x-ray tube
is 0.8o. The height of the x-ray beam
emerging from the hybrid monochromator is 1.2 mm.
Slit size and the irradiated length
Slit Marking |
Beam height (mm) |
Irradiated length (mm) |
1/2o |
1.2 |
1.2 / sin(w) |
1/4o |
0.6 |
0.6 / sin(w) |
1/8o |
0.3 |
0.3 / sin(w) |
1/16o |
0.15 |
0.18 / sin(w) |
w - angle between the
incident beam and the sample surface.