Lesson 2
Diffractometers
Nicola Döbelin
RMS Foundation, Bettlach, Switzerland
October 03 – 05, 2016, Maastricht, NL
Repetition: Generation of X-rays / Diffraction
2
Characteristic X-radiation
Anode
Target Sample
SEM: BSE detector, BSED / SAED detector
SEM: SE detector
SEM: EDX detector
EMPA: EDX / WDX
XRF
XPS
XRD (WAXS)
SAXS, XRR
Absorption:
XAS, EXAFS, XANES
3
Repetition: Generation of X-rays
Wavelength (nm)
Inte
nsity
0.00 0.05 0.10 0.15 0.20 0.25 0.30
Cu
Kα1
Kα2
Kβ
Kβ absorption filter
Monochromator Crystal
Digital filtering
Repetition: Powder Diffraction
4
n ∙ λ = 2 ∙ d ∙ sin(θ)
d
λ
θ θ 2θ
(120)
(100)
(010)
Powder sample
Repetition: Powder Diffractometer
5
X-ray tube
Primary Beam
Powder
Sample
Diffraction Cones
«Secondary Beams»
X-ray Detector scanning X-ray intensity
vs. 2θ angle
Analogue Cameras
6
http://adias-uae.com
Debye-Scherrer Camera:
Powder in Glass Capillary
Diffraction pattern recorded
on photographic film
2θ angle
Various alternative setups:
Gandolfi …
Guinier …
Straumanis …
Bradley …
Seemann-Bohlin …
…Camera
Digital Diffractometers
7
Transmission Geometry
Glass Capillary
Foil
Fluid Cell
Capillaries are ideal for:
• Light atoms (Polymers, Pharmaceuticals)
• Small amounts
• Hazardous materials
• Air-sensitive materials
Use characteristic radiation with low absorption coefficient
Flat powder sample
Reflective Geometry
Reflective Geometry is ideal for:
• Absorbing materials (Ceramics, Metals)
• Thin films
• Texture analysis
Use characteristic radiation with high absorption coefficient
Bragg-Brentano Parafocusing Diffractometer
8
Tube and Detector move symmetrically
Sample
X-ray Tube
Detector
Start
Scan
End
Instruments
9
Lab Instrument Monochromator Configuration
RMS Foundation Bruker D8 Energy dispersive Detector
Bragg-Brentano (Reflection) Debye-Scherrer (Capillary)
Uni Bern Panalytical X’Pert Ni-Filter Bragg-Brentano (Reflection)
Uni Bern Panalytical CubiX Graphite Monochromator
Bragg-Brentano (Reflection)
Bruker D8 Panalytical X’Pert Panalytical CubiX
Bragg-Brentano Diffractometer
10
Flat powder sample
More optical elements are required
to control the beam pattern.
X-ray tube
Detector
Kβ filter
Sample holder
Sample surface
Irradiated area
Primary
beam
Bragg-Brentano Parafocusing Diffractometer
11
Sample
X-ray
tube
Detector
Goniometer
circle
Divergence
slit
Soller
slit
Soller
slit
Anti-Scatter
slit
Beam
mask
Anti-Scatter
slit
Receiving
slit
Focusing
circle
Kβ Filter
Typical Configuration (with Kβ filter)
Bragg-Brentano Parafocusing Diffractometer
12
Sample
Detector
Soller
slit Anti-Scatter
slit
Receiving
slit
Secondary
monochromator
Typical Configuration (with secondary monochromator)
Modern instruments are modular.
Configuration can be changed easily.
PANalytical: «PreFIX»
Bruker: «SNAP-LOCK»
Beam Divergence
13
Divergence Slit
Soller Slit
Beam Masks
Instrument Configuration
Many optical elements = many options to
optimize data quality
How to find the best configuration?
14
Tube
Soller Slits
Programmable
Divergence Slit
Beam Mask
Sample Stage
«Spinner»
Anti-Scatter
Slit
Programmable
Anti-Scatter Slit
Soller Slits
Ni-Filter
Detector
Optimum Settings: Divergence Slit
15
80° 2θ
20° 2θ
20° 2θ
80° 2θ
Beam overflow!
- Wrong peak intensities
- Artifact signal from sample holder
Reduced beam
divergence angle
Optimum Settings: Divergence Slit
16
20° 2θ 80° 2θ
Low incident angle:
- Low penetration depth
- Large illuminated area
High incident angle:
- Deep penetration depth
- Small illuminated area
Fixed divergence slit:
Irradiated Volume
is constant
Constant intensity of
diffraction pattern
20° 2θ
Low incident angle:
- Narrow divergence slit
- Low penetration depth
Variable divergence slit:
80° 2θ
High incident angle:
- Wide divergence slit
- Deep penetration depth
Irradiated Area
is constant
Higher diffracted intensity
at high 2θ angle
Fixed vs. Variable Divergence Slit
17
20 30 40 50 60 70 80 90
Inte
nsity [a
.u.]
Diffraction Angle [°2]
fixed
variable
More than 2x higher
intensity at 90° 2θ
with variable DS
Divergence Slit: Irradiated Length
18
30.2 30.3 30.4 30.5 30.6 30.7
0
500
1000
1500
2000
2500
3000
Inte
nsity [co
un
ts]
Diffraction Angle [°2]
5mm
10mm
15mm
Soller Slits: 0.02 rad, Beam Mask: 10mm
30.2 30.3 30.4 30.5 30.6 30.7
0
20
40
60
80
100
Inte
nsity [%
]
Diffraction Angle [°2]
5mm
10mm
15mm
15 mm
10 mm
5 mm
Optimum Settings: Divergence Slit
19
Sample holder
Sample surface
Irradiated area
Primary
beam
Correct! Wrong! Wrong!
Reduce «irradiated length»
of divergence slit Use a smaller Beam Mask
Beam Mask
Beam Mask
20
30.2 30.3 30.4 30.5 30.6 30.7
0
500
1000
1500
2000
2500
3000
3500
Inte
nsity [co
un
ts]
Diffraction Angle [°2]
5mm
10mm
20mm
Soller Slits: 0.02 rad, Irradiated Length: 10mm
30.2 30.3 30.4 30.5 30.6 30.7
0
20
40
60
80
100
Inte
nsity [%
]
Diffraction Angle [°2]
5mm
10mm
20mm20 mm
10 mm
5 mm
Optimum Settings: Divergence Slit
21
Using sample holders of various sizes?
Match your Divergence Slit and Beam Mask!
Or else: Waste of intensity Beam spill-over or
30.2 30.3 30.4 30.5 30.6 30.7
0
20
40
60
80
100
Inte
nsity [%
]
Diffraction Angle [°2]
0.02rad
0.04rad
Soller Slits / Collimators
22
30.2 30.3 30.4 30.5 30.6 30.7
0
1000
2000
3000
4000
5000
6000
7000
Inte
nsity [co
un
ts]
Diffraction Angle [°2]
0.02rad
0.04rad
In primary & secondary beam, Beam Mask: 10mm, Irradiated Length: 10mm
0.04 rad
0.02 rad
Receiving Slit / Detector Slit
23
Al2O3, 15 mm irradiated length, 2.5° soller slit
34.9 35.0 35.1 35.2 35.3 35.4
0
1000
2000
3000
4000
5000
6000
7000
Inte
nsity [co
un
ts]
Diffraction Angle [°2]
0.075 mm
0.225 mm
0.375 mm
34.9 35.0 35.1 35.2 35.3 35.4
0
20
40
60
80
100
Inte
nsity [%
]
Diffraction Angle [°2]
0.075 mm
0.225 mm
0.375 mm
Summary: Monochromators
24
Optical Element Effect on Spectrum Effect on Intensity
Kβ Filter Reduces Kβ peaks Moderate loss
Graphite Monochromator Eliminates Kβ peaks Eliminates Fluorescence
Strong loss
Multi-bounce Monochromator Eliminates Kβ and Kα2 Eliminates Fluorescence
Massive loss (mostly used on Synchrotrons)
Energy dispersive Detector Reduces Kβ peaks Eliminates Fluorescence
No loss
Cu Radiation
Kβ absorption filter
filtered Radiation
Cu Radiation
Monochromator Crystal
(Graphite, d = 0.3352 nm)
CuKα1/2 Radiation
Cu Radiation Energy dispersive
Detector
Digital filtering
Summary: Optical Elements
25
Optical Element Effect Too Small Too Large
Divergence Slit Adjusts beam length on the sample
Loss of intensity Beam spills over sample
Soller Slit Reduces peak asymmetry
Loss of intensity, Better resolution
More asymmetry, Less resolution
Anti-Scatter Slit Reduces background signal
Loss of intensity High background
Beam Mask Adjusts beam width on the sample
Loss of intensity Beam spills over sample
Receiving Slit Adjusts peak width / resolution
Loss of intensity Better resolution
Loss of resolution Higher intensity
Kβ Filter Reduces Kβ peaks - -
Graphite Monochromator
Eliminates Kβ peaks - -
Bragg-Brentano Parafocusing Diffractometer
26
Sample
X-ray
tube
Detector
Detectors
27
Detector’s
window
Receiving
slit
Point Detector (0D) Linear Detector (1D) Area Detector (2D)
Receiving slit
determines
active height
Linear array of
solid state
detectors
2D array of
solid state
detectors
Scintillation counter (various)
SOL-XE (Bruker)
XFlash (Bruker)
X’Celerator (PANalytical)
PIXcel1D (PANalytical)
LynxEye (Bruker)
LynxEye XE (Bruker)
Våntec-1 (Bruker)
D/teX Ultra (Rigaku)
PIXcel3D (PANalytical)
Våntec-500 (Bruker)
SOL-XE:
Energy dispersive
XFlash:
Combines XRD + XRF
Fast
LynxEye XE:
Energy dispersive
Fast
2D image of
Debye rings
Detector
Type
Example
Key
Features
Position-sensitive
«bins»
Instruments
28
Lab Instrument Monochr. Detector
RMS Foundation Bruker D8 Energy dispersive Detector
1D LynxEye XE
Uni Bern Panalytical X’Pert Ni-Filter 1D X’Celerator
Uni Bern Panalytical CubiX Graphite 0D Scintillation Counter
Bruker D8 Panalytical X’Pert Panalytical CubiX
10 20 30 40 50 60
0
20
40
60
80
100In
ten
sity [%
]
Diffraction Angle [°2theta]
Measurement parameters
29
• Angular Range
• Step Size
• Counting Time
0 10 20 30 40 50 60
0
2000
4000
6000
8000
10000
12000
14000
Inte
nsity [C
ou
nts
]
Diffraction Angle [° 2theta]
Angular Range
30
Start before first peak
End at ≥ 60° (higher = better)
Typical Ranges:
5-60° 2θ
Angular Range
31
0 10 20 30 40 50 60
0
5000
10000
15000
20000
Inte
nsity [C
ou
nts
]
Diffraction Angle [° 2theta]
Avoid the primary beam!
Angular Range
32
0 10 20 30 40 50 60
0
5000
10000
15000
20000
25000
30000
Inte
nsity [C
ou
nts
]
Diffraction Angle [° 2theta]
No need to measure
empty background
35.0 35.1 35.2 35.3
0
5000
10000
15000
20000
25000
Inte
nsity [C
ou
nts
]
Diffraction Angle [° 2theta]
Step Size
33
At least 5 data
points per peak
Typically ≤ 0.02° 2θ
Here: 0.0122°
Time per Step
34
10 20 30 40 50 60
0
1000
2000
3000
4000
5000
6000
7000
Inte
nsity [co
un
ts]
Diffraction Angle [°2theta]
10 20 30 40 50 60
0
20
40
60
80
100
120
140
160
180
Inte
nsity [co
un
ts]
Diffraction Angle [°2theta]
12.5 min 12.5 min
1D Energy dispersive Detector 0D Detector
Examples
35
30 31 32 33 34 35
0
1000
2000
3000
4000
5000
6000
7000
Inte
nsity [co
un
ts]
Diffraction Angle [°2theta]
30 31 32 33 34 35
0
20
40
60
80
100
120
140
160
180
Inte
nsity [co
un
ts]
Diffraction Angle [°2theta]
Jagged peak shape
Noise or peak?
No recommendation!
Check your S/N ratio and peak shape!
Data Quality Checklist
36
Sample
X-ray
tube
Detector Divergence
slit
Soller
slit
Soller
slit
Anti-Scatter
slit
Beam
mask
Anti-Scatter
slit
Receiving
slit
Kβ Filter
Check beam paths Tube Sample Detector
Data Quality Checklist
37
Optical Element Ideal setup
Divergence Slit Automatic Max irr. length w/o beam overflow
Soller Slit Installed Small opening
Mask Installed (if available) Max irr. width w/o beam overflow
Anti-scatter slit Identical to divergence slit
Sample Spinning
Anti-scatter slit Wide open
Soller slit Installed Small opening
Additional slits Wide open
Kβ filter Installed
For linear detector with Kβ filter
Incid
en
t b
ea
m p
ath
D
iffr
acte
d b
eam
path