TEST OF A CONFOCAL MULTILAYER

Slides:



Advertisements
Similar presentations
X-rays Long Wave IR Visible UV X-rays Gamma rays wavelength (nm) Frau Röntgen's hand.
Advertisements

Application Report Dr. Ya-Ching Yang phone: (02) #205
Focusing monochromators/analyzers Asymmetric diffraction geometry of the monochromator Dispersive double crystal monochromator Two wavelength sandwich.
Plan : lattices Characterization of thin films and bulk materials using x-ray and electron scattering V. Pierron-Bohnes IPCMS-GEMME, BP 43, 23 rue du Loess,
X-ray sources Sealed tubes - Coolidge type common - Cu, Mo, Fe, Cr, W, Ag intensity limited by cooling req'ments (2-2.5kW) Sealed tubes - Coolidge type.
Are your X-ray powder diffraction patterns any good? Are your X-ray powder diffraction patterns any good?
ContrAA ® - A Revolution in Spectroscopy Basics and Applications of High-Resolution Continuum Source AAS.
Instrumentation - making & detecting x-rays Read Roe - Chap 2 through (ignore neutrons)
Problems with Bragg-Brentano diffractometer geometry Multilayer optics.
Effective lens aperture Deff
ITAM CAS, IEAP CTU IWORID 2004Glasgow, th July IWORID 2004 OPTIMIZATION OF X ‑ RAY DYNAMIC DEFECTOSCOPY USING MEDIPIX-2 FOR HIGH FRAME RATE READ-OUT.
Chapter 12 Atomic X-Ray Spectroscopy
FP7 FMTXCT Project UMCE-HGUGM second year activity report Partner FIHGM Laboratorio de Imagen Médica. Medicina Experimental Hospital Universitario Gregorio.
Rayleigh Scattering Mapping System School of Physics, University of Western Australia Australia – Italy Workshop on GW Detection 2005.
X-Ray Diffraction Dr. T. Ramlochan March 2010.
PHYS 430/603 material Laszlo Takacs UMBC Department of Physics
Other modes associated with SEM: EBIC
LPROT Experiment TE/MPE/PE EN/STI EN/MME. Objectives Create the conditions to produce hydrodynamic tunneling. Benchmarking FLUKA-BIG2 simulations. Assert.
X-Ray Measurement Methods From Chapter 6 of Textbook 2 and other references Diffractometer Hull/Debye-Scherrer method Pinhole method Laue Method Rotating.
Assessing Single Crystal Diamond Quality
Motor driven incident slits (define the incident x-ray beam size) Synchrotron x-ray upstream beam aperture CCD camera Video camera Long working distance.
Plan : lattices Characterization of thin films and bulk materials using x-ray and electron scattering V. Pierron-Bohnes IPCMS-GEMME, BP 43, 23 rue du Loess,
1 Data Acquisition What choices need to be made?.
Stability Requirements for Superconducting Wiggler Beamlines
X-ray powder diffractometer X-ray powder diffractometer.
X-ray diffraction and minerals. Is this mineral crystalline?
R. Pani Department of Experimental Medicine and Pathology University of Rome La Sapienza-Italy. Flat Panel PMT: advances in position sensitive photodetection.
G. Ferioli, R. Jung - LHC-BI Review Workshop November 19&20 LHC Screen Profile Monitors G. Ferioli, R. Jung Introduction BTV LHC layout Monitor set-up.
Parameters of the new diffractometer “ARES” Aleksey E. Sokolov PNPI NRC “KI”
X-ray diffraction for today and tomorrow
Essential Parts of the Diffractometer X-ray Tube: the source of X Rays Incident-beam optics: condition the X-ray beam before it hits.
Prepared By – Amit $hah M.Pharm 1 st sem QA Roll NO :- 03 Guided By – Mr. Pinak R. Patel Assistant Professor Dept. P’ceutical Chem. D Dharmaj Degree Pharmacy.
Soft Materials Research Center (SMRC) facilities Major Capabilities – Structural analysis X-ray diffraction facility Freeze-fracture transmission electron.
Crystallite Size Determination: A Comparison of Methods and Approaches Mark Light & Sarah Clark, University of Southampton UK Abstract A number of treated.
Optical Characterization and Performances of Aerogel Radiator L.Barion, G.Battaglia, M. Contalbrigo, P. Lenisa, A.Movsisyan, L. Pappalardo, M. Turisini.
1 Yi-Pai HuangAdvanced Display Optics Lab 學研計畫 --- 子計畫二 掃描式光學元件 --- 多電極液晶透鏡 Speaker: Yi-Pai Huang ( 黃乙白教授 ) Department of Photonics and Display Institute,
X-ray Crystallography - The Beginning
Outline ・ Introduction ・ XRD experiment by the SOPHIAS detector
Low Temperature Phase Transitions in GdPdAl
1. Detector 2. Crystal diffraction conditions
CHARACTERIZATION OF THE STRUCTURE OF SOLIDS
Temperature Dependence of Lattice Parameters
X-ray studies of Spincrossover Compounds in the LIEST State
ß-Eucryptite, a phase with many open questions
Temperature Dependence of Lattice Parameters
Visit for more Learning Resources
Testing and Calibration at IHEP for eXTP (current plans and needed facilities) YuSa Wang
X-ray Single Crystal Study of Na0.5Bi0.5TiO3
Diffraction Literature:
X-ray diffraction and NMR spectroscopy of Rb3DxH1-x(SO4)2
M. RIESTER , H. BÖHM and V. PETRICEK‡ contact:
ROTAN the X-Ray laboratory Daniel Šimek Jan Drahokoupil Zbyněk Šourek
X-ray Scattering from Thin Films
C. David, IEEE Conference, Rome,
What did I learn in school today?
X-ray powder diffractometer.
Quality of the radiographic image
Status of Equatorial CXRS System Development
X-ray powder diffractometer.
Basic of Light & Optics
Crystal and X-ray Diffraction
Semiconductor Detectors
Optics John Arthur, SLAC & William W. Craig, LLNL April 24, 2002
Essential Parts of the Diffractometer X-ray Tube: the source of X Rays Incident-beam optics: condition the X-ray beam before it hits.
Computed Tomography (C.T)
Gain measurements of Chromium GEM foils
What if you use a capillary, small specimen or transmission technique
Experience with photoinjector at ATF
SAXS Laboratory Instrumentation
Option 1: Reduced FF Quad Apertures
Presentation transcript:

TEST OF A CONFOCAL MULTILAYER "Confocal Max-FluxTM Optic", OSMIC Inc., Troy, Michigan, USA J. Schneider Elektrotechnik GmbH, D-77652 Offenburg, Germany References Powder sample A powder sample (Si-powder) in a capillary (Ø = 0.3 mm) is placed at the position of the single crystal. MoKa Graphite monochromator CuKa OSMIC Optic Comparison of two Foci Size mm2 Power kW/mA Powerdensity kW/mm2 Intensity counts 0.1x1 1.2/34 12 2900 0.3x3 3/85 3.3 4100 Ratio 2.5 0.23 1.44 Focus test with an ENRAF-NONIUS rotating anode CuKa, 35 kV Variation of the Distance d from the Optic 430 mm 490 690 430 460 540 590 640 740 mm 430 mm, a steel sphere of 0.5 mm Image of the single reflection double reflection Distance = 430 mm, pixel size 62.5 mm Monochromator Confocal graded multilayer optic of OSMIC ®Inc. Focus Technical Data from the data sheet of OSMIC ®Inc : Major radius a: 502.5 mm Minor radius b: 11.8 mm Position of the mirror : -202.5 mm Length of the optic : 100 mm Focal to focal distance: 1005 mm Distance between Source and optic : 300 mm side – by – side geometry horizontal beam geometry (45 ° inclination) at 90 mm at 180 mm Comparison Intensity of reflections from a crystal sphere ( Ø = 0.25 mm) for different positions D of the optic and for a graphite monochromator G versus the intensity without a monochromator D / amplification D = 600 / 12.8 D = 500 / 8.0 D = 400 / 5.6 G D = 400 / 1.1 Experimental Set-up 300 mm D =390 – 700 mm 40 - 350 mm X – ray Source Crystal Detector CCD Camera Scintillation Counter d Intensity versus Distance The variation of the maximum intensity: measured intensity , intensity corrected for absorption in air. The variation of the maximum intensity corrected for absorption in air for the two line foci X-Ray Source SCHNEIDER® Rotating Anode Generator: Mo – and Cu –Radiation, 5.5 kW Spot Focus: 0.3 x 3 mm2 Intensity for different values of the bias voltage [V] Pin-hole image Scan of the Beam: Profile Slit of the detector was put into two positions; scan was performed by moving the slit in the indicated direction beam Detector slit d=500 Movement D of the slit 1 2 d = 500 mm d = 550 mm FWHM Acknowledgment: The work is financially supported by the Materialwissenschaftliches Forschungszentrum der Johannes-Gutenberg-Universität Mainz and by the "Deutsche Forschungsgemeinschaft" Bonn TEST OF A CONFOCAL MULTILAYER X-RAY OPTIC Joachim Kusz and Horst Böhm Institute of Physics, University of Silesia, Katowice, Poland Institut für Geowissenschaften, Johannes Gutenberg-Universität Mainz, D-55099 Mainz, Germany. The performance of the multilayer optic : Optimum performance for a spot focus 0.3 x 3 mm Homogeneous profile for D > 500 mm Optimum crystal position with maximum gain depends on the size of the crystal (flexible positioning of the diffractometer). Sharp lines with high resolution for powder samples (very useful with a CCD detector for materials with big lattice parameters) Precise determination of lattice parameters for single crystals. Useful application for metric changes at phase transitions Measurements of diffuse intensities. Measurements of sputtered thin films . Conclusion