Shining Synchrotron Light on Supercritical Fluids Alan J. Anderson St. Francis Xavier University.

Slides:



Advertisements
Similar presentations
Raman Spectroscopy A) Introduction IR Raman
Advertisements

Spectroscopy Photoelectron spectroscopy X-ray absorption spectroscopy
FLAME SPECTROSCOPY The concentration of an element in a solution is determined by measuring the absorption, emission or fluorescence of electromagnetic.
Pressure-Induced Polymerization of 24NHBn(Dehydro[24]annulenes) Shimizu-group M1 NAKASE Tomoya 1.
Specific heat Blue=olivine, green=MgO, orange=forsterite, black=Al2O3, brown=grossular, purple=pyrope, red=CaO.
Catalysis and Catalysts - XPS X-Ray Electron Spectroscopy (XPS)  Applications: –catalyst composition –chemical nature of active phase –dispersion of active.
Atomic X-Ray Spectroscopy Chapter 12 X-ray range  Å to 100 Å Used  0.1Å to 25 Å.
Fundamental Techniques and Measurements  Mass Measurements  Volume Measurements  Preparation of a solution of known concentration  UV-Visible Spectrophotometer.
X Ray Flouresence Analysis (XRF). XRF X-Ray Fluorescence is used to identify and measure the concentration of elements in a sample X-Ray Fluorescence.
GeoSoilEnviroCARS Matt Newville, Steve Sutton, Mark Rivers Applications: XANES EXAFS Techniques: Near-neighbor distances and coordination environment.
Pushing the limits of IR …an update of new possibilities in CLS spectroscopy Ferenc Borondics CAP Meeting 2011, St. John’s, NL.
X-Ray Photoelectron Spectroscopy (XPS)
Scanning Electron Microscope Jamie Goings. Theory Conventional microscopes use light and glass lenses SEM uses electrons and magnetic lenses to create.
ED and WD X-ray Analysis
Towards X-ray excited optical microscopy (XEOM) for cultural heritage, spectroelectrochemistry, and wider applications Mark Dowsett 1, Annemie Adriaens.
Advanced Photon Source. GeoSoilEnviroCARS Operate a national user facility at the APS for the conduct of frontier experiments in earth, planetary,
20-Jun-2003  XRF and  XAFS with the GSECARS X-ray Microprobe Matthew Newville, Steve Sutton, Mark Rivers, Peter Eng, Tom Trainor Consortium for Advanced.
Ge 116 Module 1: Scanning Electron Microscopy
Lecture 5 An Introduction to Spectroscopy Electromagnetic radiation, electromagnetic wave Emission, absorption, fluorescence.
Chem. 133 – 3/10 Lecture. Announcements I Exam 1 –Average (66.5) + Distribution –A little worse than average Today’s Lecture –Electrochemistry (just questions)
etc… Analysing samples with complex geometries Particles Inclusions
Synchrotron Radiation Interaction with Matter; Different Techniques Anders Nilsson Stanford Synchrotron Radiation Laboratory What can we hope to learn?
X-Ray Diffraction Spectroscopy RAMAN Microwave. What is X-Ray Diffraction?
Joachim Stöhr Stanford Synchrotron Radiation Laboratory X-Ray Absorption Spectroscopy J. Stöhr, NEXAFS SPECTROSCOPY,
Introduction Techniques Conclusions Contamination control on bulk Ge and GaAs As dopants in Ge S Monolayer passivation on Ge Si passivation and HfO 2 dielectric.
Seminar Author: Bojan Hiti Mentor: doc. dr. Matjaž Kavčič Determination of trace impurities on Si wafers with x-ray fluorescence.
1 M. Aslam Baig National Center for Physics Quaid-i-Azam University Campus, Islamabad Pakistan
R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.
Surface Analysis Surface interface controls many aspects of chemistry
Advanced Spectroscopy 3. Infrared Spectroscopy. Revision 1.What molecular or structural features give rise to absorption of infrared (IR) radiation? covalent.
Five Slides about X-ray Photoelectron Spectroscopy (XPS) Created by Sophia Hayes (Washington University, Sarah St. Angelo (Dickenson.
Effective lens aperture Deff
What are the key ingredients for a successful laser heating experiment at the synchrotron? Guoyin Shen CARS, University of Chicago GeoSoilEnviroCARS The.
Investigation of fluid- fluid phase transition of hydrogen under high pressure and high temperature 2014/11/26 Shimizu laboratory SHO Kawaguchi.
Nano-Materials Characterization Yoram Shapira, EE Nano-bio-electronics Growth and Processing Characterization and Analysis Design and Modeling.
Chapter 12 Atomic X-Ray Spectroscopy
A U.S. Department of Energy Office of Science Laboratory Operated by The University of Chicago Argonne National Laboratory Office of Science U.S. Department.
Electrical conduction property of solid iodine in the molecular phase Shimizu Group Yu TANAKA.
A XAS Study of the Sulphur Environment Location in Human Neuromelanin and Synthetic Analogues P.R. Crippa, M. Eisner, S. Morante, F. Stellato, F. Vicentin,
Nuclear Instrumentation Laboratory Federal University of Rio de Janeiro -BRAZIL X-ray Fluorescence and X-ray Transmission Microtomography Imaging System.
CLS Status Update E. Matias Canadian Light Source.
Scanning tunneling microscopy (STM) Atomic force microscopy (AFM) Scanning electrochemical microscopy (SECM) UV & visible spectroscopy Transmission experiments.
Other modes associated with SEM: EBIC
Susanna Guatelli & Barbara Mascialino G.A.P. Cirrone (INFN LNS), G. Cuttone (INFN LNS), S. Donadio (INFN,Genova), S. Guatelli (INFN Genova), M. Maire (LAPP),
In situ chemichromic studies of interactions between a lutetium bis-octaalkyl-substituted phthalocyanine and selected biological cofactors by C. Pal, A.
Ljubljana, July 2011 Physics on synchrotrons and computers Alojz Kodre Faculty of Math & Physics, University of Ljubljana.
X-ray spectroscopy Andrew Preston
Department of Synchrotron Radiation Research Lund University
Paul Northrup Brookhaven National Laboratory
Stability Requirements for Superconducting Wiggler Beamlines
NANO 225 Intro to Nano/Microfabrication
Atomic Fluorescence Spectroscopy. Background l First significant research by Wineforder and Vickers in 1964 as an analytical technique l Used for element.
Heterometallic Carbonyl Cluster Precursors Heterometallic molecular cluster precursor - mediate transport and growth of nanoscale bimetallic particles.
Synthesis and characterization of poorly-crystaline Fe-Al nano- hydroxides Crop and Soil Sciences Department & Center of Environmental Kinetics Analysis.
X-ray absorption spectroscopy (XAS)
Scanning tunneling microscopy (STM) Atomic force microscopy (AFM) Scanning electrochemical microscopy (SECM) UV & visible spectroscopy Transmission experiments.
Characterization of CsI:Tl recrystalization after liquid phase deposition Ulrik Lund Olsen, Ph.D. student supervisors: H.F. Poulsen, S. Schmidt SCINT’07,
Supercritical Fluid Assisted Particle Synthesis Antoinette Kretsch New Jersey Institute of Technology.
Date of download: 6/7/2016 Copyright © 2016 SPIE. All rights reserved. X-ray diffraction (XRD) data and Raman spectra of TiO2 NS (a) and (c) and TiO2 NR.
EXAFS-spectroscopy method in the condensed matter physics: First results on energy-dispersive EXAFS station in RSC “Kurchatov Institute” Vadim Efimov Joint.
RAMAN EFFECT.
Satish Pradhan Dnyanasadhana College Department Of Chemistry
Anezka Radkova, Heather Jamieson
Australian Nuclear Science and Technology Organisation, Australia
Extending IBA Analysis:
Kinetics of Phase Transformations
Satish Pradhan Dnyanasadhana College Department Of Chemistry
mXRF and mXAFS with the GSECARS X-ray Microprobe
FLAME SPECTROSCOPY The concentration of an element in a solution is determined by measuring the absorption, emission or fluorescence of electromagnetic.
Raman Spectroscopy A) Introduction IR Raman
Presentation transcript:

Shining Synchrotron Light on Supercritical Fluids Alan J. Anderson St. Francis Xavier University

The Hydrothermal Diamond Anvil Cell HDAC

Hydrothermal Diamond Anvil Cell (HDAC)

Grooves Sample Chamber Re Gasket Different Diamond Anvil Configurations

Surface Profilometry Average depth μm Volume 3.55 X 10 6 µm 3 FIB Milling of Diamond Anvil

Aqueous solution Vapor bubble HDAC Sample Chamber at 25 o C 0.2 mm

Liquid Vapor Isochores ρ = 0.87

Synchrotron X-ray Micro- and Nanoprobes

Canadian Light Source Inc.

Detector

VaporLiquid Path of Incident X-rays Path of Fluorescence X-rays to the Detector Solution in Sample 25 ºC 300 µm Diamond Anvil

X-ray Fluorescence Imaging and Quantitative Analysis

Map showing the distribution of Ta 2 O 5 particles in 5% HF at 25 ºC (HDAC 116) Map showing the distribution of Ta in 5% HF at 360°C (HDAC 116) Solid Ta 2 O 5 Particles 100 µm

Ta 2 O 5 Dissolved in 5% HF HDAC 360°C (ρ = 0.566) 10,700 μg mL -1 Ta HDAC 350°C (ρ = 0.575) 7,400 µg mL -1 Ta Ta Standard (1000 µg mL -1 ) HDAC 360°C (ρ = 0.575) HDAC 400°C (ρ = 0.504) Ta L β1 Fe K β1 Fe K α1 Ta L α1 Energy (keV) Intensity

Time resolved analysis - Pb in aqueous fluid during interaction with partially metamict zircon (ZrSiO 4 ) at 300 o C

X-ray Absorption Spectroscopy XAS Resolving the local structure of metals in SCW

X-ray Absorption Fine Structure (XAFS)

Summary Synchrotron – based techniques Monitor SCW – material interaction Resolve the local structure of aqueous metal complexes Solubility of selected oxides

Raman spectroscopy Raman system HDAC on the microscope

Energy (keV) Re L lines Ta L lines Interferences in X-ray Emission Spectra

Energy (keV) Counts Sample Contamination from Re Gasket

CH 4 Sample Contamination from Gasket Reaction with Diamond

X-ray Diffraction

In situ XRD Wu et al. (1997) Dehydration & Rehydration of Montmorillonite Reversible changes in lattice dimensions