2015 Cameca Users Meeting KαKα K L M Fluorescence and absorption… A sample of olivine has Fe, Mg and Si. Fe K α = 6.4 keV Binding energies… Mg K = 1.30.

Slides:



Advertisements
Similar presentations
Giuseppe Dalba, La Fisica dei Raggi X, Dipartimento di Fisica, Università di Trento, a.a Transmission MATTER Scattering Compton Thomson Photoelectric.
Advertisements

Aurélien Moy Claude Merlet (UM2/GM)
Saeedeh Ghaffari Nanofabrication Fall 2011 April 15 1.
X-ray Diffraction. X-ray Generation X-ray tube (sealed) Pure metal target (Cu) Electrons remover inner-shell electrons from target. Other electrons “fall”
EDX-Spectra Simulation
UWO Nanofabrication Facility and Science Studio. Facility to be hooked into Science Studio: Western Nanofabrication Facility, University of Western Ontario.
Hong Koh Yiin -CAMTEC Image from:
X-Ray Microanalysis - Determination of Elemental Concentration How do we get from counts to concentration? ElementWt.% Ti29.9 Fe35.8 Mn2.82 O31.3 total99.82.
LCLS Atomic Physics with Intense X-rays at LCLS Philip H. Bucksbaum, University of Michigan, Ann Arbor, MI Roger Falcone, University of California, Berkeley,
Spectrum Identification & Artifacts Peak Identification.
Trace Element Abundances in Single Presolar SiC Stardust Grains by Synchrotron X-Ray Fluorescence (SXRF) Zhonghu Cai (XOR) Barry Lai (XOR) Steve Sutton.
Catalysis and Catalysts - XPS X-Ray Electron Spectroscopy (XPS)  Applications: –catalyst composition –chemical nature of active phase –dispersion of active.
K-Shell Spectroscopy of Au Plasma Generated with a Short Pulse Laser Calvin Zulick [1], Franklin Dollar [1], Hui Chen [2], Katerina Falk [3], Andy Hazi.
ED and WD X-ray Analysis
Interactions with Matter
Qualitative, quantitative analysis and “standardless” analysis NON DESTRUCTIVE CHEMICAL ANALYSIS Notes by: Dr Ivan Gržetić, professor University of Belgrade.
etc… Analysing samples with complex geometries Particles Inclusions
Corpuscular induced and X-ray or γ -ray induced fluorescence NON DESTRUCTIVE CHEMICAL ANALYSIS Notes by: Dr Ivan Gržetić, professor University of Belgrade.
X-Ray Fluorescence Analysis by Gergana Hristozova Project supervisor: s. eng. M. Gustova FLNR.
Radiation therapy is based on the exposure of malign tumor cells to significant but well localized doses of radiation to destroy the tumor cells. The.
X - Rays & Crystals Characterizing Mineral Chemistry & Structure J.D. Price Characterizing Mineral Chemistry & Structure J.D. Price.
Photoemission Fundamentals of Data Acquisition and Analysis J. A. Kelber, June Texts: PHI handbook, Briggs and Seah Outline: I.Photoemission process.
John Fournelle Eugene Cameron Electron Microprobe Lab Department of Geology and Geophysics University of Wisconsin - Madison Monte Carlo Simulations and.
Surface Analysis Surface interface controls many aspects of chemistry
Atomic Absorption Spectroscopy
The Hot Plasma in the Galactic Center with Suzaku Masayoshi Nobukawa, Yoshiaki Hyodo, Katsuji Koyama, Takeshi Tsuru, Hironori Matsumoto (Kyoto Univ.)
Quantitative Analysis Quantitative analysis using the electron microprobe involves measuring the intensities of X-ray lines generated from your unknown.
Anomalous Small-Angle X-ray Scattering Beamline B1 at HASYLAB, DESY MM Ulla Vainio 1, Günter Goerigk 2, Rainer Gehrke 1 1 HASYLAB at DESY, Notkestr.
Ion Beam Analysis Dolly Langa Physics Department, University of Pretoria, South Africa Blane Lomberg Physics Department, University of the Western Cape,
Precision Analysis of Electron Energy Deposition in Detectors Simulated by Geant4 M. Bati č, S. Granato, G. Hoff, M.G. Pia, G. Weidenspointner 2012 NSS-MIC.
FRANK LABORATORY OF NEUTRON PHYSICS ION BEAM ANALYSIS STANCIU-OPREAN LIGIA SUPERVISOR DR. KOBZEV ALEXANDER.
Space Instrumentation. Definition How do we measure these particles? h p+p+ e-e- Device Signal Source.
Financial Consulting Group 0 © 2010 ООО "Группа Финансового Консультирования", компания, зарегистрированная в соответствии с законодательством Российской.
The Influence of the Return Current and the Electron Beam on the X-Ray Flare Spectra Elena Dzifčáková, Marian Karlický Astronomical Institute of the Academy.
Pbio550: Biophysics of Ca2+ signaling ( washington
Xspress3 Tests Dec-2014 Comparisons of: GSE ME-4 Vortex, 350um thick sensor, older pre-amp. APS ME-4 Vortex, 1000um thick sensor, newer ASIC pre-amp. using.
Shining Synchrotron Light on Supercritical Fluids Alan J. Anderson St. Francis Xavier University.
The Problem of Secondary Fluorescence in EPMA in the Application of the Ti-in-Zircon Geothermometer And the Utility of PENEPMA Monte Carlo Simulations.
Plan : intro Characterization of thin films and bulk materials using x-ray and electron scattering V. Pierron-Bohnes IPCMS-GEMME, BP 43, 23 rue du Loess,
ENDF/B-VI Coupled Photon-Electron Data for Use in Radiation Shielding Applications by Dermott E. Cullen Lawrence Livermore National Laboratory & Robert.
2015 Cameca Users Meeting Background characterization – must account for background shape Curvature Spectrometer efficiency Natural Bremsstrahlung shape.
SEM- Schematic Overview. Electron Detection Tungsten Filament Electron Source.
Gamma ray interaction with matter A) Primary interactions 1) Coherent scattering (Rayleigh scattering) 2) Incoherent scattering (Compton scattering) 3)
Example of the output produced by XRF
1.1 What’s electromagnetic radiation
The probe Some material used from:. EPMA - electron probe microanalysis Probe signals.
1 Activation by Medium Energy Beams V. Chetvertkova, E. Mustafin, I. Strasik (GSI, B eschleunigerphysik), L. Latysheva, N. Sobolevskiy (INR RAS), U. Ratzinger.
Interactions of Ionizing Radiation
X-ray Fluorescence Physics of XRF Characteristics Caveats Instrumentation.
Jiaxin Wang and Robin P. Gardner Oct 6 th 2011, CEAR at NC State University, Raleigh, NC.
Sunil Kumar, Namita yadav, Pragya Bhatt, Raj Singh, B. K. Singh, R
Lecture 4a Common Error in EPMA: Secondary Fluorescence from Outside Primary Excitation Volume John Fournelle, Ph.D. Department of Geoscience University.
The Problem of Secondary Fluorescence in EPMA in the Application of the Ti-in-Zircon Geothermometer And the Utility of PENEPMA.
BUCKY Simulations of Z and RHEPP Experiments
International Workshop on radiosensitization
of interfaces in glass/crystal composites for nuclear wasteforms
Electron probe microanalysis EPMA
Electron Probe Microanalysis EPMA
Pamela Aaron, Dr. Charles Shearer, and Paul Burger
Electron probe microanalysis EPMA
Atomic Absorption Spectroscopy
Today’s take-home lessons: FRET (i. e
Research Co-ordination Meeting of the IAEA CRP on “Elements of power
Atomic Absorption Spectroscopy. Atomic absorption spectroscopy is based on the same principle as the flame test used in qualitative analysis.
LSP Modeling of Ultra-Intense Lasers on Cone-Coupled Wire Targets:
ION BEAM ANALYSIS.
Electron probe microanalysis - Scanning Electron Microscopy EPMA - SEM
The Geant4 Hadrontherapy Advanced Example
Tryptophan - gas phase tautomer
Presentation transcript:

2015 Cameca Users Meeting KαKα K L M Fluorescence and absorption… A sample of olivine has Fe, Mg and Si. Fe K α = 6.4 keV Binding energies… Mg K = 1.30 keV Si K = 1.84 keV Fe Kα excites both Si Kα and Mg Kα, resulting in “too much” intensity for Mg and Si, meanwhile, the Fe Kα intensity decreases due to absorption by Si and Mg, resulting in “too little” intensity of Fe… However, Fe LIII edge (binding energy) = 707 eV reduces Mg Kα and Si Kα intensities, so competing factors!

2015 Cameca Users Meeting Fe-Ca silicate Fe-Ca sil. Ca Kα Fluorescence at a distance… Fe silicate High energy Fe Kα fluoresces Ca Kα in adjacent phase. Analysis “sees” Ca at this beam position.

2015 Cameca Users Meeting Fluorescence range

The difficult problem of boundary fluorescence… Electrons may not go far, but X-rays do 2015 Cameca Users Meeting

The difficult problem of boundary fluorescence… More blank testing… Line or grid acquisition: Most analyses will be wrong! 20 μm Th Mα 6.31+/ / / Monazite Th concentration 2015 Cameca Users Meeting

Penepma Francesc Salvat and Xavier Llovet

2015 Cameca Users Meeting Mid 1990s = code system PENELOPE 2000s = EPMA related main program PENEPMA Simulates X-ray emission spectra Computationally very lengthy, so not suitable for real-time data processing

2015 Cameca Users Meeting Fast calculation - semi-analytical method developed Use physical interaction parameters from PENELOPE numerical database Use primary photon intensities obtained by short MC simulation runs to create parameter files for each material in a boundary couple X-ray intensity with distance is modelled, which permits the estimation of k-ratios and calculated concentrations resulting from fluorescence.

2015 Cameca Users Meeting

Petrology of Chromite in Ureilites: Implications for Primary Petrogenesis and Secondary Processes –C.A. Goodrich et al

2015 Cameca Users Meeting rutile Ti K edge =4.96 keV La Lβ =5.04 keV monazite

2015 Cameca Users Meeting rutile

2015 Cameca Users Meeting

Rutile inclusions

2015 Cameca Users Meeting