Analysis of Iron Oxidation in Garnets By, Erica A. Emerson By, Erica A. Emerson.

Slides:



Advertisements
Similar presentations
Unit 1.3 Nuclear Chemistry
Advertisements

When an nucleus releases the transition energy Q (say 14.4 keV) in a  -decay, the  does not carry the full 14.4 keV. Conservation of momentum requires.
NUCLEAR CHEMISTRY The Basics. The Nucleus The nucleus is composed of nucleons –protons –neutrons A nucleus is characterized by two numbers –atomic mass.
Catalysis and Catalysts - XPS X-Ray Electron Spectroscopy (XPS)  Applications: –catalyst composition –chemical nature of active phase –dispersion of active.
Forsterite Crystal Myanmar. Olivine structure c b M2 M1 Two cation sites: M1 M2.
Measuring the Temperature of Hot Solar Flare Plasma with RHESSI Amir Caspi 1,2, Sam Krucker 2, Robert P. Lin 1,2 1 Department of Physics, University of.
Neutral Particles. Neutrons Neutrons are like neutral protons. –Mass is 1% larger –Interacts strongly Neutral charge complicates detection Neutron lifetime.
Lesson 9 Gamma Ray Decay. Electromagnetic decay There are two types of electromagnetic decay,  -ray emission and internal conversion (IC). In both of.
A. Dokhane, PHYS487, KSU, 2008 Chapter2- Nuclear Fission 1 Lecture 3 Nuclear Fission.
6-1 RFSS: Lecture 6 Gamma Decay Part 2 Readings: Modern Nuclear Chemistry, Chap. 9; Nuclear and Radiochemistry, Chapter 3 Energetics Decay Types Transition.
Radiology is concerned with the application of radiation to the human body for diagnostically and therapeutically purposes. This requires an understanding.
Several nomenclatures are important: ● Nuclide: is any particular atomic nucleus with a specific atomic number Z and mass number A, it is equivalently.
When an nucleus releases the transition energy Q (say 14.4 keV) in a  -decay, the  does not carry the full 14.4 keV. Conservation of momentum requires.
Joachim Stöhr Stanford Synchrotron Radiation Laboratory X-Ray Absorption Spectroscopy J. Stöhr, NEXAFS SPECTROSCOPY,
Corey Thompson Technique Presentation 03/21/2011
Nuclear Energy. Nuclear energy is all around us and can be used for medical purposes. Nuclear energy is when an atom is split and releases energy or particles.
Mossbauer Spectroscopy
Chapter 2 The composition and Structure of the Atom Denniston Topping Caret 4 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required.
Text here Chapter 5. Atoms Atoms are the smallest particle of at element that have the properties of that element. Atoms are too small to be seen with.
Atomic Structure and Radiation REVIEW GAME
Nuclear Chemistry.
Mössbauer spectroscopy References: J.P. Adloff, R. Guillaumont: Fundamentals of Radiochemistry, CRC Press, Boca Raton, 1993.
Nuclear Chemistry.
Honors Forensic Science.  Introduction  Organic substances constitute a substantial portion of physical evidence submitted to crime labs  Carbon does.
Alpha, Beta, and Gamma Decay
6- PRENTICE HALL ©2007 Pearson Education, Inc. Upper Saddle River, NJ CRIMINALISTICS An Introduction to Forensic Science, 9/E By Richard Saferstein.
Atomic Spectroscopy for Space Applications: Galactic Evolution l M. P. Ruffoni, J. C. Pickering, G. Nave, C. Allende-Prieto.
Atomic Theory and Structure Chapters 4-5 Atomic Theories Democritus ~ 400 BC believed that atoms were indivisible and indestructible Dalton ~ 1800’s.
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,
Gamma Decay Energetics Decay Types Transition Probabilities
THE NUCLEUS: A CHEMIST’S VIEW. Nuclear Symbols Element symbol Mass number, A (p + + n o ) Atomic number, Z (number of p + )
NE Introduction to Nuclear Science Spring 2012 Classroom Session 3: Radioactive Decay Types Radioactive Decay and Growth Isotopes and Decay Diagrams.
Topic 2 Atomic Theory SL+HL. Topic 2.1 The atom Position ChargeRelative Mass Proton; p + Nucleus 1+ 1 Neutron; n Nucleus 0 1 Electron; e - Cloud/orbitals.
1.3-1 Types of Radioactivity.  By the end of this section you will be able to: ◦ Observe nuclear changes and explain how they change an element. ◦ Express.
List the following electromagnetic spectrum wave types in order from lowest energy to highest energy: Gamma rays Infrared Microwaves Radiowaves Ultraviolet.
List the following electromagnetic spectrum wave types in order from lowest energy to highest energy: Gamma rays Infrared Microwaves Radiowaves Ultraviolet.
The nucleus consists of protons and neutrons, collectively called nucleons. The number of protons is the atomic number. Protons plus neutrons is the atomic.
Radioactivity.
Topic 2 Atomic Theory SL+HL. Topic 2.1 The atom Position ChargeRelative Mass Proton; p + Nucleus 1+ 1 Neutron; n Nucleus 0 1 Electron; e - Cloud/orbitals.
UEQ Where does the concept and understanding of the atom originate?
Radiometric Dating Continuation of Journal Entry #5.
INTRODUCTION The oxidation state of iron indicates the amount of oxygen present when a mineral is formed. If the environment was abundant in oxygen, many.
Mass Spectroscopy Introduction.
Electron Energy Loss Spectroscopy (EELS) Suggested Reading: Used electron spectrometer Used TEM Review of theory for elastic + inelastic scattering Examples.
Chapter 29:Nuclear Physics
Nuclear Physics.
A Brief Review of “Matter”. Atom nucleus electron e-e- (proton,neutrons) p+p+ n ● 10,000,000 atoms can fit across a period in your textbook. ● The nucleus.
1 Mössbauer Effect J-H. Kim
C-4 Atomic Structure The nucleus and the moving electrons.
Mineral Spectroscopy Visible Infrared Raman Mössbauer NMR.
Nuclear Chemistry. Radioactivity The process by which materials give off such rays radioactivity; the rays and particles emitted by a radioactive source.
Nuclear Symbols Element symbol Mass number (p + + n o ) Atomic number (number of p + )
Unstable Nuclei and Radioactive Decay Radioactivity – spontaneous emission of radiation Radiation – rays and particles emitted from a radioactive material.
Mass Spectrometry Molecular weight can be obtained from a very small sample. It does not involve the absorption or emission of light. A beam of high-energy.
Welcome to the X-Ray Absorption Fine Structure Online Orientation! This orientation will provide you with tips that will help you conduct a successful.
Welcome to the X-Ray Absorption Fine Structure Online Orientation! This orientation will provide you with tips that will help you conduct a successful.
Laser manipulation of nuclear transitions: experiment.
Jun Hee Cho1, Sang Gil Ko1, Yang kyu Ahn1, Eun Jung Choi2
Mossbauer spectroscopy
University of Ioannina
Mössbauer spectroscopy
ANALYSIS OF IRON OXIDATION IN GARNETS
DO NOW Pick up notes sheet and Subatomic particle table.
CHEM 312: Lecture 6 Part 2 Gamma Decay
Introduction Spectroscopy is an analytical technique which helps determine structure. It destroys little or no sample. The amount of light absorbed by.
° status report analysis details: overview; “where we are”; plans: before finalizing result.. I.Larin 02/13/2009.
The fingerprints of elements
Ion-beam, photon and hyperfine methods in nano-structured materials
Atomic Spectra As atoms gain energy their electrons can be excited and absorb energy in discrete amounts called quanta and produce absorption spectrums.
° status report analysis details: overview; “where we are”; plans: before finalizing result.. I.Larin 02/13/2009.
Presentation transcript:

Analysis of Iron Oxidation in Garnets By, Erica A. Emerson By, Erica A. Emerson

Order of Events  Goals of this study  Brief introduction of research conducted  Major results  Mössbauer  XANES  Conclusions  Questions  Goals of this study  Brief introduction of research conducted  Major results  Mössbauer  XANES  Conclusions  Questions

Goals of this study  Measure recoil-free fractions for Fe 2+ and Fe 3+ and use those results to measure Fe 3+ accurately on a suite of 20 garnets by Mössbauer  Use XANES on same samples to calculate the % Fe 3+, and then compare it to Mössbauer results.  Measure recoil-free fractions for Fe 2+ and Fe 3+ and use those results to measure Fe 3+ accurately on a suite of 20 garnets by Mössbauer  Use XANES on same samples to calculate the % Fe 3+, and then compare it to Mössbauer results.

Introduction: Iron Oxidation and Relation to fo 2  Oxidation state is a description of how many electrons it has lost or gained from its original state  If the environment was abundant in oxygen, many of the minerals in the assemblage will contain oxidized iron, Fe 3+.  If the environment is more reducing, there is likely to be more Fe 2+.  Oxygen fugacity (fo 2 ) is measure of the amount of free or uncombined oxygen available in an environment  Oxidation state is a description of how many electrons it has lost or gained from its original state  If the environment was abundant in oxygen, many of the minerals in the assemblage will contain oxidized iron, Fe 3+.  If the environment is more reducing, there is likely to be more Fe 2+.  Oxygen fugacity (fo 2 ) is measure of the amount of free or uncombined oxygen available in an environment

 The amount of each depends largely on the oxidation conditions, hence on the oxygen fugacity  High fo 2 => Fe 3+  Low fo 2 => Fe 2+  Really Low fo 2 => Fe 0  Presence of oxygen in a magma results in crystallization of different minerals  The amount of each depends largely on the oxidation conditions, hence on the oxygen fugacity  High fo 2 => Fe 3+  Low fo 2 => Fe 2+  Really Low fo 2 => Fe 0  Presence of oxygen in a magma results in crystallization of different minerals

Effect of Oxidation State of Iron on Crystallization (basaltic magmas)

Mössbauer and XANES  Mössbauer spectroscopy  A technique based on the discovery of recoilless gamma ray emission and absorption discovered in  Radioactive isotope ( 57 Co) breaks down into a stable isotope ( 57 Fe). As the radioactive source breaks down it, releases gamma rays known as beta decay.  Used to identify and quantify Fe 2+ /Fe 3+ ratios in garnets.  XANES (X-ray Absorption Near-edge Structure)  A synchrotron transmits photons into the samples (Calas et al., 1987).  The photon energy then excites electrons within the sample, resulting in low-probability, localized transitions of the K-level, 1s, to partially-filled or lowest-energy, empty, bound, excited states (Calas et al and Dyar et al. 2002).  Measure the transmitted light and changes in energy  Mössbauer spectroscopy  A technique based on the discovery of recoilless gamma ray emission and absorption discovered in  Radioactive isotope ( 57 Co) breaks down into a stable isotope ( 57 Fe). As the radioactive source breaks down it, releases gamma rays known as beta decay.  Used to identify and quantify Fe 2+ /Fe 3+ ratios in garnets.  XANES (X-ray Absorption Near-edge Structure)  A synchrotron transmits photons into the samples (Calas et al., 1987).  The photon energy then excites electrons within the sample, resulting in low-probability, localized transitions of the K-level, 1s, to partially-filled or lowest-energy, empty, bound, excited states (Calas et al and Dyar et al. 2002).  Measure the transmitted light and changes in energy

Mössbauer spectra displaying Fe 3+ in andradite garnet. Andradite, pure garnet, courtesy of Val Malenko. Mössbauer spectrum displaying Fe 2+ in a Fort Wrangell almandine garnet. MIT Teaching collection. Mössbauer Results  Error Analysis  Temperature error was  1K  Isomer shift and quadrupole splitting error was  0.02 mm/s

 Temperature series of this sample was acquired (4-295K)  Calculated recoil-free fraction, f and C to obtain accurate Fe 3+ /Fe 2+ percentages.

 Recoil calculation  Corrects for energy loss due to recoil  Allows for accurate and true measurement of %Fe 3+  Calculation and significance of C  C value compares f (Fe 3+ ) and f (Fe 2+ )  Used to calculate cations of Fe 2+ and Fe 3+ per formula unit  Recoil calculation  Corrects for energy loss due to recoil  Allows for accurate and true measurement of %Fe 3+  Calculation and significance of C  C value compares f (Fe 3+ ) and f (Fe 2+ )  Used to calculate cations of Fe 2+ and Fe 3+ per formula unit Mössbauer Spectroscopy

XANES Results  Error Analysis  Pre-edge peak extraction in using X26A Data Plotter resulted in the error of  0.03 eV.  PAN: Peak Analysis and resulted in an error of  0.1 eV.  Error on peak position is thus at least  0.13 eV  Probably depends on extent of peak overlap  and peak multiplicity

Mössbauer Fe 3+ vs. XANES Fe 3+ Except for sample bbkg and 9b, results agree within ±5% absolute!

Mössbauer Fe 3+ vs. XANES Fe 3+ Best fit line to data 1:1 line

Conclusions  As a reminder: The goal of this study was to measure the oxidation states of garnets using the Mössbauer and XANES techniques.  The percentages of Fe 3+ and Fe 2+ according to Mössbauer and XANES, revealing that both techniques agree well within ±5%, with the exception of samples AK97-9b and the Kenyan melanite.  In conclusion, the Mössbauer spectroscopy and XANES results complement each other. Mössbauer and XANES data measure approximately the same percentage of Fe 3+ content.  As a reminder: The goal of this study was to measure the oxidation states of garnets using the Mössbauer and XANES techniques.  The percentages of Fe 3+ and Fe 2+ according to Mössbauer and XANES, revealing that both techniques agree well within ±5%, with the exception of samples AK97-9b and the Kenyan melanite.  In conclusion, the Mössbauer spectroscopy and XANES results complement each other. Mössbauer and XANES data measure approximately the same percentage of Fe 3+ content.