new possibilities for xray difractometry...new 2d - quazar multilayer optics • low maintenance •...
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NEW POSSIBILITIES FOR X-RAY DIFFRACTOMETRY
Bernd Hasse – Incoatec, Geesthacht, Germany
This document was presented at PPXRD -Pharmaceutical Powder X-ray Diffraction Symposium
Sponsored by The International Centre for Diffraction Data
This presentation is provided by the International Centre for Diffraction Data in cooperation with the authors and presenters of the PPXRD symposia for the express purpose of educating the scientific community.
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B. Hasse – PPXRD 2009, Glasgow2/22
Bright sealed tube for ultimate convenience
Incoatec Microfocus Source – IµS
The source
• Point focus sealed tube
• Cu, Mo, Cr, or Ag anode
• High brilliance
• Low power: 30 W
• Air-cooled
• Tube change as easy as for conventional sealed-tubes
• 3 Years warranty
B. Hasse – PPXRD 2009, Glasgow3/22
Optimized Optics in Incoatec‘s new very stable and easy-to-align housing
Incoatecs Microfocus Source – IµS
The optics and housing
• New family of 2D beam shapingMontel Optics: The Quazar Optics
• 2D focusing or collimating or hybrid (f+c)
• Patented housing with optional motors
• Stable positioning
B. Hasse – PPXRD 2009, Glasgow4/22
New Equipment for Diffractometry
Microfocus Source IµS
Optics with Housing
Sample stage
2D detector(VÅNTEC 2000)
Bruker D8 GADDSwith IµSTM
B. Hasse – PPXRD 2009, Glasgow5/22
IµSTM & VÅNTEC-2000
• symmetrical reflection
• 600 sec collection time
• sample to detector 15 cm
Sample: quartz powder
B. Hasse – PPXRD 2009, Glasgow6/22
D8 Discover with GADDS
IµSTM & VÅNTEC-2000
°2θ
The five fingers of quartz
B. Hasse – PPXRD 2009, Glasgow7/22
IµSTM for XRD with focusing optics
• measurements in transmission geometry
• with Bruker D8 GADDS and VÅNTEC 2000
B. Hasse – PPXRD 2009, Glasgow8/22
IµS (Cu-Kα) with focusing optics vs. classical setup
IµS – 2D focussing optics
• Spotsize 230 µm
• 0.3 mm snout
• small slice for integration to obtain better resolution (poor detector calibration)
15 sec collection time
Ibuprofen / measured in transmission geometry / Sample-Detector distance 290 mm
Sealed Tube – 1D collimating optics
• 0.3 mm collimator
120 sec collection time
B. Hasse – PPXRD 2009, Glasgow9/22
IµSTM focusing onto the detector: LaB6
FW HM of LaB6 sample fitted with PV function
403938373635343332313029282726252423222120
105,000100,000
95,00090,00085,00080,00075,00070,00065,00060,00055,00050,00045,00040,00035,00030,00025,00020,00015,00010,000
5,0000
-5,000
0.09174322 0.07588469 0.08700313
60 seconds, 292 mm sample-detector
FWHM: 0.08°2θ
B. Hasse – PPXRD 2009, Glasgow10/22
D8 DISCOVER with GADDS HTS (IµS):Combinatorial Screening Reflection & Transmission
B. Hasse – PPXRD 2009, Glasgow11/22
IµS (Cu-Kα) with collimating optics for SAXS measurementsSilver behanate (H3C-(CH2)20-COOAg) / Bruker AXS NANOSTAR / 3-Pinhole-geometry / 1000 s exposure time / 1035 mm detector distance
q
Total Intensity: 17.000 cps (IµS @ 30W)
For comparison:Sealed tube with cc-Göbel mirrors @ 1.4 kW: 3.300 cps
B. Hasse – PPXRD 2009, Glasgow12/22
IµS with a marDTB
B. Hasse – PPXRD 2009, Glasgow13/22
ASS with Cu-Kα
Whole tabletExposure time: 300 sFocusing onto the detector
B. Hasse – PPXRD 2009, Glasgow14/22
Temperature-dependent Phase Transition in Copper phthalocyanine
N
N
N
N
N
N
N NCu
• Heating from 30 °C to 350 °C with a rate of 0.75 K/min• Exposure time per frame: 240 s• Operation mode of mar345: 100 µm x 100 µm @ 240 mm
R.E. Dinnebier, M. Müller, MPI for Solid State Research, Stuttgart
B. Hasse – PPXRD 2009, Glasgow15/22
Results• Reaction Temperature:
- TR = 295 °C (Lab data)- TR = 275 °C (Synchrotron data)
• Activation Energy: - EA = 254 kJ·mol-1 (Lab data)- EA = 245 kJ·mol-1 (Synchrotron data)Calculated with the non-isothermal Avrami-theorie- EA = 241 kJ·mol-1 (isothermal investigation)
R.E. Dinnebier, M. Müller, MPI for Solid State Research, Stuttgart
B. Hasse – PPXRD 2009, Glasgow16/22
IµS (Mo-Kα) with focusing optics: LaB6
Frame integrated with Powder3DIPProfile Matching with FullProf
<FWHM> = 0.13°2θ
Sample-Detector Distance: 260 mm2θ: 30°Slitsize: 0.2 x 0.2 mm²Spot size: 110 µmExposure time: 1200 s
B. Hasse – PPXRD 2009, Glasgow17/22
Ibuprofen with Mo-Kα
Whole tablet in blister packExposure time: 120 sFocusing onto the detector
**
***
B. Hasse – PPXRD 2009, Glasgow18/22
Comparison of IµS (Mo-Kα) and IµS (Ag-Kα)
Mo Ag
End of measurement range for Mo-Kα
Sample: LaB6Exposure Time:
300 sDetector-Distance:
200 mm
B. Hasse – PPXRD 2009, Glasgow19/22
IµS (Ag-Kα) with focusing optics: Pigment Red 170 in diamond anvil cell
Exposure time: 1200 s
M. Schmidt, Uni Frankfurt/M; K. Friese, A. Grzechnik, Uni Bilbao
B. Hasse – PPXRD 2009, Glasgow20/22
Summary (1): XRD with IµS
Incoatec Microfocus Source IµS
• Microfocus Source• 30 W, air-cooled• New 2D - Quazar
Multilayer Optics• Low maintenance• for Cu, Mo, Cr, and Ag
B. Hasse – PPXRD 2009, Glasgow21/22
• 2D focusing beam• XRD in transmission• Well plate screening• Position sensitive
measurements• Single crystal
diffraction
Summary (2): XRD with IµS
• 1D collimating beam +1D focusing beam
• XRD in reflection• Texture• Phase identification
• 2D collimating beam• SAXS• Texture
Acknowledgement
All colleagues @ Incoatec GmbH
M. Schmidt, Frankfurt/M, Germany
K. Friese, A. Grzechnik, Uni Bilbao, Spain
R.E. Dinnebier, M. Müller, MPI for Solid State Research,Stuttgart, Germany
All colleagues from Bruker AXS