SlideShare une entreprise Scribd logo
1  sur  12
Fundamental of
XAS
Presented by
Amlan Roy
Research Scholar, Department of Energy Scien
Engineering (DESE)
IIT Bombay, Powai-400076
Mumbai, India
AR
Acronym
• XAFS X-ray Absorption Fine Structure or XAS X-ray Absorption
Spectroscopy
• XANES X-ray Absorption Near Edge Structure or NEXAFS Near Edge X-ray
Absorption Fine Structure
• EXAFS Extended X-ray Absorption Fine Structure
XANES
Local Symmetry
Oxidation state
EXAFS
Bond distance
Neighbor's nature
XAFS/XAS
AR
Basic Principles
• X-ray Absorption Spectroscopy (XAS)
• Interaction of inner electron with the X-ray (involvement of the Core
electron)
• Incident x-ray energy should be higher than the binding energy of the core
e-
K-edge
L-edge
M-edge
Incoming
X-ray
e-
Vacuum level
1
2
3
4
Auger e-
1
2
3
4
Excitation of core e- by
incoming x-rays
Promotion of core e- to
vacuum level
e- transfer from higher to
lower level
Energy released in terms of
auger e-/ fluorescent x-ray
‘Photoelectric effect’
AR
Basic Principles
• Relaxation process: After excitation, the relaxation process can be done by
the demotion of electron from higher level to ground state.
X-ray Fluorescence and Auger effect
https://doi.org/10.1007/978-0-387-92897-5_1224https://jascoinc.com/learning-center/theory/fluorescence-spectroscopy/
AR
XAS
XANES EXAFS
https://en.wikipedia.org/wiki/Extended_X-ray_absorption_fine_structure
Basic Principles
https://doi.org/10.1016/j.bbamcr.2014.11.027
AR
Basic Principles
Energy range
XANES EXAFS
5-150 eV Beyond 150 eV
Kinetic energy of the photo electron,
For XANES, low energy and higher wavelength is responsible for multiple scattering
For EXAFS corresponding to single scattering
1st shell1st shell
2nd shell
single scatteringMultiple scattering
AR
• Absorption edge Energy at which sharp rise of the absorption coefficient
due to generation of photoelectron by the atom
• Threshold energy defend as the energy beyond which
continuous production of photoelectron happens
• At Absorption edge, energy of incident X-ray equal to
binding energy of the core level electron.
Basic Principles
Pre-edge linked to crystal field transition from core level to empty
higher level. The weak intensity because ∆l = 2,
• features of Transition metal in Periodic Table,
• sensitive to the metal coordination number and symmetry
XANES contains Pre-egde, Absorption edge, White line
Introduction to X-ray Absorption Spectroscopy by Bruce Ravel, Synchrotron Science Group National Institute of Standards and Technology & Beamline
for Materials Measurements National Synchrotron Light Source II, September 30, 2015
White line is the main feature in the main rise of the absorption
and mostly the highest peak. It is related to transitions of the photo
electron into the molecular orbital
AR
Monochromatic
ray
Ionization chamber Ionization chamber
DetectorI0 It
Fluorescent
Detector
Transmission
mode
Fluorescent
mode
Lambert-Beer law
If
Absorption coefficient: μ
I0 = Ite-μt where, t is the thickness of the sample
μ depends on X-ray energy E and atomic number z by the following equation:
μ = (ρz4)/(AE3) A atomic mass and ρ density
Instrumentation
AR
Fundamentals of XAFS by Matthew Newville Consortium for Advanced Radiation Sources University of Chicago, Chicago, IL
Absorption Coefficient
AR
Major synchrotron sources all over the world
X-ray Absorption Spectroscopy by J. E. PENNER-HAHN The University of Michigan, Ann Arbor, MI, USA
AR
Application
• Surface study- Thin film
• Catalysis study
• Material Science- Superconductor, Energy storage
• Solid state physics- study of single crystal
• Bioscience-bonding in Protein, peptide with ligand
Phys. Rev. B 94, 174107 REVIEW L. J. Gamble , Anal. Chem. 2006 , 78 , 3316
AR
•ADF Calculation of NEXAFS using spin-orbit coupling TDDFT or the Slater-TS
method.
•FDMNES Calculation of NEXAFS using finite difference method and full multiple
scattering theory.
•FEFF8 Calculation of NEXAFS using full multiple scattering theory.
•MXAN NEXAFS fitting using full multiple scattering theory.
•FitIt NEXAFS fitting using multidimensional interpolation approximation.
•PARATEC NEXAFS calculation using plane-wave pseudopotential approach
•WIEN2k NEXAFS calculation on the basis of full-potential (linearized) augmented
plane-wave approach.
Software for NEXAFS analysis
https://www.wikiwand.com/en/X-ray_absorption_near_edge_structure

Contenu connexe

Tendances

Mossbauer spectroscopy
Mossbauer spectroscopyMossbauer spectroscopy
Mossbauer spectroscopy
Yogesh Chauhan
 
X Ray Diffraction Spectroscopy
X Ray Diffraction SpectroscopyX Ray Diffraction Spectroscopy
X Ray Diffraction Spectroscopy
hephz
 
Auger electron spectroscopy
Auger electron spectroscopyAuger electron spectroscopy
Auger electron spectroscopy
Gulfam Hussain
 

Tendances (20)

SEM & FESEM.pptx
SEM & FESEM.pptxSEM & FESEM.pptx
SEM & FESEM.pptx
 
Mossbauer Spectroscopy
Mossbauer SpectroscopyMossbauer Spectroscopy
Mossbauer Spectroscopy
 
Mössbauer spectroscopy ppt
Mössbauer spectroscopy pptMössbauer spectroscopy ppt
Mössbauer spectroscopy ppt
 
Mossbauer Spectroscopy
Mossbauer SpectroscopyMossbauer Spectroscopy
Mossbauer Spectroscopy
 
Cyclic voltammetry
Cyclic voltammetryCyclic voltammetry
Cyclic voltammetry
 
Cyclic Voltammetry Application
Cyclic Voltammetry  Application Cyclic Voltammetry  Application
Cyclic Voltammetry Application
 
Mossbauer spectroscopy
Mossbauer spectroscopyMossbauer spectroscopy
Mossbauer spectroscopy
 
Mossbauer spectroscopy
Mossbauer spectroscopyMossbauer spectroscopy
Mossbauer spectroscopy
 
Mossbauer Spectroscopy
Mossbauer SpectroscopyMossbauer Spectroscopy
Mossbauer Spectroscopy
 
XRF Lecture Notes
XRF Lecture NotesXRF Lecture Notes
XRF Lecture Notes
 
X Ray Diffraction Spectroscopy
X Ray Diffraction SpectroscopyX Ray Diffraction Spectroscopy
X Ray Diffraction Spectroscopy
 
Cyclic Voltametery
Cyclic VoltameteryCyclic Voltametery
Cyclic Voltametery
 
X ray powder diffraction
X ray powder diffractionX ray powder diffraction
X ray powder diffraction
 
Auger electron spectroscopy
Auger electron spectroscopyAuger electron spectroscopy
Auger electron spectroscopy
 
Difference b/w electron, neutron and X-ray diffraction and advantages
Difference b/w electron, neutron and X-ray diffraction and advantagesDifference b/w electron, neutron and X-ray diffraction and advantages
Difference b/w electron, neutron and X-ray diffraction and advantages
 
Electron spectroscopy
Electron spectroscopyElectron spectroscopy
Electron spectroscopy
 
Xps (x ray photoelectron spectroscopy)
Xps (x ray photoelectron spectroscopy)Xps (x ray photoelectron spectroscopy)
Xps (x ray photoelectron spectroscopy)
 
Mxenes presentation.pptx
Mxenes presentation.pptxMxenes presentation.pptx
Mxenes presentation.pptx
 
XRF Theory and Application
XRF Theory and ApplicationXRF Theory and Application
XRF Theory and Application
 
Density functional theory
Density functional theoryDensity functional theory
Density functional theory
 

Similaire à Basic Introduction of XANES and EXAFS

PHYSICS GROUP- 5 UV Spectroscopy for nanomaterials.pptx
PHYSICS GROUP- 5 UV Spectroscopy for nanomaterials.pptxPHYSICS GROUP- 5 UV Spectroscopy for nanomaterials.pptx
PHYSICS GROUP- 5 UV Spectroscopy for nanomaterials.pptx
dbhansali57
 
Introduction To Spectroscopy
Introduction To SpectroscopyIntroduction To Spectroscopy
Introduction To Spectroscopy
guest824336
 
Aip pg book of abstracts
Aip pg book of abstractsAip pg book of abstracts
Aip pg book of abstracts
Siddartha Verma
 

Similaire à Basic Introduction of XANES and EXAFS (20)

Presentation on environmental science notes
Presentation on environmental science notesPresentation on environmental science notes
Presentation on environmental science notes
 
X ray spectroscopy. ppt
X ray spectroscopy. ppt X ray spectroscopy. ppt
X ray spectroscopy. ppt
 
Uv
UvUv
Uv
 
light emission spectroscopy,raman spectroscopy, flourimetry,flame photometry,...
light emission spectroscopy,raman spectroscopy, flourimetry,flame photometry,...light emission spectroscopy,raman spectroscopy, flourimetry,flame photometry,...
light emission spectroscopy,raman spectroscopy, flourimetry,flame photometry,...
 
Laser Functions
Laser FunctionsLaser Functions
Laser Functions
 
Perovskite
PerovskitePerovskite
Perovskite
 
PHYSICS GROUP- 5 UV Spectroscopy for nanomaterials.pptx
PHYSICS GROUP- 5 UV Spectroscopy for nanomaterials.pptxPHYSICS GROUP- 5 UV Spectroscopy for nanomaterials.pptx
PHYSICS GROUP- 5 UV Spectroscopy for nanomaterials.pptx
 
uv visible spectroscopy.pptx
uv visible spectroscopy.pptxuv visible spectroscopy.pptx
uv visible spectroscopy.pptx
 
Analysis of Thermoplastic by using Spectroscopic Technique
Analysis of Thermoplastic by using Spectroscopic TechniqueAnalysis of Thermoplastic by using Spectroscopic Technique
Analysis of Thermoplastic by using Spectroscopic Technique
 
Quang phổ cầm tay
Quang phổ cầm tayQuang phổ cầm tay
Quang phổ cầm tay
 
Introduction To Spectroscopy
Introduction To SpectroscopyIntroduction To Spectroscopy
Introduction To Spectroscopy
 
Analytical Spectroscopic systems
Analytical Spectroscopic systemsAnalytical Spectroscopic systems
Analytical Spectroscopic systems
 
Solid stateppt (1)
Solid stateppt (1)Solid stateppt (1)
Solid stateppt (1)
 
Crabtree_2012
Crabtree_2012Crabtree_2012
Crabtree_2012
 
Raman spectroscopy- General Talak
Raman spectroscopy- General TalakRaman spectroscopy- General Talak
Raman spectroscopy- General Talak
 
Field Ion - Infrared- Raman Spectroscopy
Field Ion - Infrared- Raman SpectroscopyField Ion - Infrared- Raman Spectroscopy
Field Ion - Infrared- Raman Spectroscopy
 
2019 hm-iv-pixe
2019 hm-iv-pixe2019 hm-iv-pixe
2019 hm-iv-pixe
 
Raman Spectroscopy.pdf
Raman Spectroscopy.pdfRaman Spectroscopy.pdf
Raman Spectroscopy.pdf
 
Aip pg book of abstracts
Aip pg book of abstractsAip pg book of abstracts
Aip pg book of abstracts
 
Fundamentals of spectroscopy
Fundamentals of spectroscopyFundamentals of spectroscopy
Fundamentals of spectroscopy
 

Dernier

Cloud Frontiers: A Deep Dive into Serverless Spatial Data and FME
Cloud Frontiers:  A Deep Dive into Serverless Spatial Data and FMECloud Frontiers:  A Deep Dive into Serverless Spatial Data and FME
Cloud Frontiers: A Deep Dive into Serverless Spatial Data and FME
Safe Software
 

Dernier (20)

Navigating the Deluge_ Dubai Floods and the Resilience of Dubai International...
Navigating the Deluge_ Dubai Floods and the Resilience of Dubai International...Navigating the Deluge_ Dubai Floods and the Resilience of Dubai International...
Navigating the Deluge_ Dubai Floods and the Resilience of Dubai International...
 
Apidays New York 2024 - The Good, the Bad and the Governed by David O'Neill, ...
Apidays New York 2024 - The Good, the Bad and the Governed by David O'Neill, ...Apidays New York 2024 - The Good, the Bad and the Governed by David O'Neill, ...
Apidays New York 2024 - The Good, the Bad and the Governed by David O'Neill, ...
 
Apidays New York 2024 - APIs in 2030: The Risk of Technological Sleepwalk by ...
Apidays New York 2024 - APIs in 2030: The Risk of Technological Sleepwalk by ...Apidays New York 2024 - APIs in 2030: The Risk of Technological Sleepwalk by ...
Apidays New York 2024 - APIs in 2030: The Risk of Technological Sleepwalk by ...
 
Apidays New York 2024 - Passkeys: Developing APIs to enable passwordless auth...
Apidays New York 2024 - Passkeys: Developing APIs to enable passwordless auth...Apidays New York 2024 - Passkeys: Developing APIs to enable passwordless auth...
Apidays New York 2024 - Passkeys: Developing APIs to enable passwordless auth...
 
MS Copilot expands with MS Graph connectors
MS Copilot expands with MS Graph connectorsMS Copilot expands with MS Graph connectors
MS Copilot expands with MS Graph connectors
 
TrustArc Webinar - Unlock the Power of AI-Driven Data Discovery
TrustArc Webinar - Unlock the Power of AI-Driven Data DiscoveryTrustArc Webinar - Unlock the Power of AI-Driven Data Discovery
TrustArc Webinar - Unlock the Power of AI-Driven Data Discovery
 
presentation ICT roal in 21st century education
presentation ICT roal in 21st century educationpresentation ICT roal in 21st century education
presentation ICT roal in 21st century education
 
Apidays New York 2024 - Accelerating FinTech Innovation by Vasa Krishnan, Fin...
Apidays New York 2024 - Accelerating FinTech Innovation by Vasa Krishnan, Fin...Apidays New York 2024 - Accelerating FinTech Innovation by Vasa Krishnan, Fin...
Apidays New York 2024 - Accelerating FinTech Innovation by Vasa Krishnan, Fin...
 
Cloud Frontiers: A Deep Dive into Serverless Spatial Data and FME
Cloud Frontiers:  A Deep Dive into Serverless Spatial Data and FMECloud Frontiers:  A Deep Dive into Serverless Spatial Data and FME
Cloud Frontiers: A Deep Dive into Serverless Spatial Data and FME
 
Apidays New York 2024 - Scaling API-first by Ian Reasor and Radu Cotescu, Adobe
Apidays New York 2024 - Scaling API-first by Ian Reasor and Radu Cotescu, AdobeApidays New York 2024 - Scaling API-first by Ian Reasor and Radu Cotescu, Adobe
Apidays New York 2024 - Scaling API-first by Ian Reasor and Radu Cotescu, Adobe
 
Rising Above_ Dubai Floods and the Fortitude of Dubai International Airport.pdf
Rising Above_ Dubai Floods and the Fortitude of Dubai International Airport.pdfRising Above_ Dubai Floods and the Fortitude of Dubai International Airport.pdf
Rising Above_ Dubai Floods and the Fortitude of Dubai International Airport.pdf
 
Platformless Horizons for Digital Adaptability
Platformless Horizons for Digital AdaptabilityPlatformless Horizons for Digital Adaptability
Platformless Horizons for Digital Adaptability
 
EMPOWERMENT TECHNOLOGY GRADE 11 QUARTER 2 REVIEWER
EMPOWERMENT TECHNOLOGY GRADE 11 QUARTER 2 REVIEWEREMPOWERMENT TECHNOLOGY GRADE 11 QUARTER 2 REVIEWER
EMPOWERMENT TECHNOLOGY GRADE 11 QUARTER 2 REVIEWER
 
Six Myths about Ontologies: The Basics of Formal Ontology
Six Myths about Ontologies: The Basics of Formal OntologySix Myths about Ontologies: The Basics of Formal Ontology
Six Myths about Ontologies: The Basics of Formal Ontology
 
Polkadot JAM Slides - Token2049 - By Dr. Gavin Wood
Polkadot JAM Slides - Token2049 - By Dr. Gavin WoodPolkadot JAM Slides - Token2049 - By Dr. Gavin Wood
Polkadot JAM Slides - Token2049 - By Dr. Gavin Wood
 
Exploring Multimodal Embeddings with Milvus
Exploring Multimodal Embeddings with MilvusExploring Multimodal Embeddings with Milvus
Exploring Multimodal Embeddings with Milvus
 
Mcleodganj Call Girls 🥰 8617370543 Service Offer VIP Hot Model
Mcleodganj Call Girls 🥰 8617370543 Service Offer VIP Hot ModelMcleodganj Call Girls 🥰 8617370543 Service Offer VIP Hot Model
Mcleodganj Call Girls 🥰 8617370543 Service Offer VIP Hot Model
 
MINDCTI Revenue Release Quarter One 2024
MINDCTI Revenue Release Quarter One 2024MINDCTI Revenue Release Quarter One 2024
MINDCTI Revenue Release Quarter One 2024
 
Connector Corner: Accelerate revenue generation using UiPath API-centric busi...
Connector Corner: Accelerate revenue generation using UiPath API-centric busi...Connector Corner: Accelerate revenue generation using UiPath API-centric busi...
Connector Corner: Accelerate revenue generation using UiPath API-centric busi...
 
Apidays New York 2024 - The value of a flexible API Management solution for O...
Apidays New York 2024 - The value of a flexible API Management solution for O...Apidays New York 2024 - The value of a flexible API Management solution for O...
Apidays New York 2024 - The value of a flexible API Management solution for O...
 

Basic Introduction of XANES and EXAFS

  • 1. Fundamental of XAS Presented by Amlan Roy Research Scholar, Department of Energy Scien Engineering (DESE) IIT Bombay, Powai-400076 Mumbai, India
  • 2. AR Acronym • XAFS X-ray Absorption Fine Structure or XAS X-ray Absorption Spectroscopy • XANES X-ray Absorption Near Edge Structure or NEXAFS Near Edge X-ray Absorption Fine Structure • EXAFS Extended X-ray Absorption Fine Structure XANES Local Symmetry Oxidation state EXAFS Bond distance Neighbor's nature XAFS/XAS
  • 3. AR Basic Principles • X-ray Absorption Spectroscopy (XAS) • Interaction of inner electron with the X-ray (involvement of the Core electron) • Incident x-ray energy should be higher than the binding energy of the core e- K-edge L-edge M-edge Incoming X-ray e- Vacuum level 1 2 3 4 Auger e- 1 2 3 4 Excitation of core e- by incoming x-rays Promotion of core e- to vacuum level e- transfer from higher to lower level Energy released in terms of auger e-/ fluorescent x-ray ‘Photoelectric effect’
  • 4. AR Basic Principles • Relaxation process: After excitation, the relaxation process can be done by the demotion of electron from higher level to ground state. X-ray Fluorescence and Auger effect https://doi.org/10.1007/978-0-387-92897-5_1224https://jascoinc.com/learning-center/theory/fluorescence-spectroscopy/
  • 6. AR Basic Principles Energy range XANES EXAFS 5-150 eV Beyond 150 eV Kinetic energy of the photo electron, For XANES, low energy and higher wavelength is responsible for multiple scattering For EXAFS corresponding to single scattering 1st shell1st shell 2nd shell single scatteringMultiple scattering
  • 7. AR • Absorption edge Energy at which sharp rise of the absorption coefficient due to generation of photoelectron by the atom • Threshold energy defend as the energy beyond which continuous production of photoelectron happens • At Absorption edge, energy of incident X-ray equal to binding energy of the core level electron. Basic Principles Pre-edge linked to crystal field transition from core level to empty higher level. The weak intensity because ∆l = 2, • features of Transition metal in Periodic Table, • sensitive to the metal coordination number and symmetry XANES contains Pre-egde, Absorption edge, White line Introduction to X-ray Absorption Spectroscopy by Bruce Ravel, Synchrotron Science Group National Institute of Standards and Technology & Beamline for Materials Measurements National Synchrotron Light Source II, September 30, 2015 White line is the main feature in the main rise of the absorption and mostly the highest peak. It is related to transitions of the photo electron into the molecular orbital
  • 8. AR Monochromatic ray Ionization chamber Ionization chamber DetectorI0 It Fluorescent Detector Transmission mode Fluorescent mode Lambert-Beer law If Absorption coefficient: μ I0 = Ite-μt where, t is the thickness of the sample μ depends on X-ray energy E and atomic number z by the following equation: μ = (ρz4)/(AE3) A atomic mass and ρ density Instrumentation
  • 9. AR Fundamentals of XAFS by Matthew Newville Consortium for Advanced Radiation Sources University of Chicago, Chicago, IL Absorption Coefficient
  • 10. AR Major synchrotron sources all over the world X-ray Absorption Spectroscopy by J. E. PENNER-HAHN The University of Michigan, Ann Arbor, MI, USA
  • 11. AR Application • Surface study- Thin film • Catalysis study • Material Science- Superconductor, Energy storage • Solid state physics- study of single crystal • Bioscience-bonding in Protein, peptide with ligand Phys. Rev. B 94, 174107 REVIEW L. J. Gamble , Anal. Chem. 2006 , 78 , 3316
  • 12. AR •ADF Calculation of NEXAFS using spin-orbit coupling TDDFT or the Slater-TS method. •FDMNES Calculation of NEXAFS using finite difference method and full multiple scattering theory. •FEFF8 Calculation of NEXAFS using full multiple scattering theory. •MXAN NEXAFS fitting using full multiple scattering theory. •FitIt NEXAFS fitting using multidimensional interpolation approximation. •PARATEC NEXAFS calculation using plane-wave pseudopotential approach •WIEN2k NEXAFS calculation on the basis of full-potential (linearized) augmented plane-wave approach. Software for NEXAFS analysis https://www.wikiwand.com/en/X-ray_absorption_near_edge_structure