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Introduction to the analysis of

Introduction to the analysis of

EXAFS data

EXAFS data

meneghini@fis.uniroma3.it

meneghini@fis.uniroma3.it

Carlo

(2)

XAFS_tutorial_Grado2013

Examples Manuals Software Grado_2013_XAFS_Tutorial.pdf

IFEFFIT VESTA Data Notepad++ Grado2013_XAFS_TUTORIAL a-Ge A-GeO2 Cu Cu 10K Fe_align W LCA

PDF slides: https://db.tt/UmF9HOc2

Complete directory

http://dl.dropbox.com/u/20746560/Meneghini_EXAFS-Tutorial-DUINO-2011.zip

(3)

Characteristics of a XAS spectrum

Characteristics of a XAS spectrum

Pre-edge

background

Near Edge

Region

(XANES)

Edge Energy

Post edge

atomic

background

J

um

p

µ

t

(4)

Data collection

Extraction of XAFS

structural signal:

χ

(k)

Structural refinement

Check the results

END

Preliminary data

treatment

Structural

model(s)

re vi si on re vi si on revision

XAFS ANALYSIS: from the experimental data to results

(5)

XAFS rarely gives absolute quantitative details

Optimize your

Optimize your

beamtime!

beamtime!

Choose properly the

experimental set-up &

sample preparation

Choose

properly data

collection

strategy

Check the

data quality

during the

experiment

Always measure

reference data

Proposal submission + proposal

Proposal submission + proposal

evaluation + beamtime scheduling

evaluation + beamtime scheduling

=

=

6 to 12 months 6 to 12 months !!

- Check the proposal submission deadlines, - discuss your experiment with local contacts,

- check your data during the experiment

It is difficult to

It is difficult to

obtain new beamtime

obtain new beamtime

for the same proposal

for the same proposal

in case of failure!!!! in case of failure!!!! Quality is better than quantity ELETTRA: 15-09 + 15-03 ESRF: 01-09 + 01-03 XANES/EXAFS Fluo/TEY/transmission ….

Data collection

(6)

Errors in XAFS data analysis

Errors in XAFS data analysis

are dominated by

are dominated by

systematic errors

systematic errors

:

:

--

spurious structures

spurious structures

--

background subtraction

background subtraction

--

wrong models

wrong models

--

inaccurate theory

inaccurate theory

Data collection

Experimental set-up &

sample preparation

Transmission: massive concentrated samples

inhomogeneities, holes, not parallel surfaces, etc...

Fluorescence:

thin concentrated

thick diluted samples

Self absorption, detector linearity, Bragg reflections

TEY: thick concentrated

Surface sensitivity, sample charge, Bragg reflections

a

- step scan / quick EXAFS - Fixed Energy or K steps - single scan/repeated scans - temperature points - . . .

Collection strategy

b

Data quality

S/N ratio glitches discontinuities c

IXS Standards and Criteria Subcommittee Reports

Measure reference

samples

d

1-energy calibration

2-data analysis procedures calibration

The power of XAFS technique consists in highlighting the smallest structural

(7)

-0.0006 -0.0004 -0.0002 0 0.0002 0.0004 13200 13500 13800 α(E) E (eV) 0.3 0.6 0.9 1.2 12000 12300 12600 12900 13200 13500 α(E) E (eV)

J

High degree polynomial -0.0003 -0.0002 -0.0001 0 0.0001 0.0002 0.0003 13200 13500 α(E) E (eV) 0 5 10 15 20 25 30 σ = 1.1e-4

S/N ~ J/

σ

Evaluate S/N ratio

Check

Check

regularly

regularly

during the

during the

experiment

experiment

(8)

0.3 0.6 0.9 1.2 12000 12300 12600 12900 13200 13500 α(E) E (eV)

Glitches

Discontinuities

Check systematically during the experiment

Check systematically during the experiment

edge shift

I0 I1 I2 Ref.Sample Sample Iref=ln I1/I2 Iexp=ln Io/I1
(9)

Select properly the best spectra and

useful data regions

Sum together the best spectra

Preliminary

data treatment

- Self absorption corrections -deglitching

-data interpolation - data alignement

don't use blue one!

Weighting by S/N

a b c

Absorption signal

Transmission

Fluorescence & TEY

Check carefully the

Check carefully the

data quality during

data quality during

the experiment

the experiment

Preliminary data treatment

µx<<1

Experimental set-up generally provide macros for automatic data collection over

(10)

α

=

α

O

+

α

pre

α

o

calculation

Fourier Transform

Fourier Filtering

pre

-edge

subtraction

structural signal

χ

(k)

Structural

refinement

XAFS structural signal

Absorption signal

Transmission

Fluorescence & TEY

revise preliminary

tratments

µo = free atom absorption

µ = embedded atom absorption

pre = all but the absorber

Extract

χ

(k)

structural signal

(11)

Background subtraction

calculate

µ

o

and

χ

(k)

Fourier

Transform

a

b c

pre = aE+b

(12)

Structural signal

Define E

o

µ

o

= represents the bare

atom absorption.

It is calculated empirically as a smooth curve across the data. Different XAFS data analysis

software apply different (generally equivalent) methods

Requirements for µo:

1) Smooth enough to not remove true structural features

2) Structured enough to remove background structures

k

Calculate k

Define

µ

o

Calculate

χ

(k)

Check FT

Large |FT| contributions at low (unphysical) distances may signify

"wrong µµµµo"

Note: Multiple excitations my affect

the background with (small) discontinuities

A. Di Cicco et Al. Phys. Rev. B 62, 12001 (2000)

(13)

Fourier Transform

Shape of FT widely changes

as a function of:

• FT window

• k

w

weight

• data range

k3χ(k) kχ(k) kχ(k) k3χ(k)

FT shows more intuitively

the main structural features

in the real space: the FT

modulus represent a

pseudo-radial distribution function

modified by the effct of

amplitude, phase and mean

free path parameters:

|FT| peaks point out

interatomic correlations

Peak positions are not the

true distances due to the

photoelectron phase shift

(14)

Fourier Filtering

k3χ(k)

FT

Back Fourier

transform

(BFT)

Fourier filtering allows

isolating contributions

of selected regions of

the FT

Background contribution

(15)

Choose a

model

Refine the structural

parameters: N, R,

σ

2

Select the relevant

structural contributions

add new

contributions?

Change the model?

Y

Y

END

Revise your data

extraction?

Y

Theoretical χ(k) exp fit Experimental χ(k) Exp. χ(k)

data refinement

n

n

(16)

Choose a structural model

Barns.ill.fr

Full inorganic structure

database (ICSD)

(registration

fees

)

Protein Data Base

(Free)

How to find a model

structure

How to visualize the

structure

How to calculate

distances and

geometries

http://database.iem.ac.ru/mincryst/ http://millenia.cars.aps.anl.gov/cgi-bin/atoms/atoms.cgi
(17)

ex p fit

How a data

refinement

program works

Amplitude and phase functions from atomic cluster models experimental data Theoretical formula

(18)

http://www.esrf.eu/computing/scientific/exafs/ FEFF home-page

GNXAS home-page

XAFS data analysis software

XAFS organizations

XAFS data analysis

http://feff.phys.washington.edu/feff/ http://gnxas.unicam.it http://cars9.uchicago.edu/ifeffit/ e x p f i t A m or ph ou s & d is or d er ed s ys te m s

(19)

Install Ifeffit.exe

1.

athena

GUI for Data Processing with Ifeffit

2.

artemis

GUI for XAFS Fitting with Ifeffit

3.

hephaestus

GUI for general x-ray properties of the elements

4.

sixpack

GUI for XAFS Processing and Fitting with Ifeffit

5.

feff6L

Stand-alone program for ab inito EXAFS calculations

6.

atoms

Stand-alone, command line crystallography->feff.inp

7.

autobk

Stand-alone background removal program

8.

feffit

Stand-alone FEFF fitting program

9.

ifeffit

command-line version of Ifeffit

advantages:

•Freeware, multiplatform (Win, Mac, Linux) • easy to handle, • semi-automatic procedures

drawbacks:

• easy to handle, • semi-automatic procedures

Ifeffit.exe

(20)

Inside the Ifeffit directory

Manuals and Manuals and tutorials tutorials

Estract

Estract

χ(k

χ

(k

)

)

data fitting

data fitting

Info on the

Info on the

proposed

proposed

example

example

Database of

Database of

crystallographic

crystallographic

structures as *.

structures as *.

inp

inp

files for

files for

Atoms

Atoms

Configuration files:

Configuration files:

NOT FOR NEWBIES

(21)

Data collection

Extraction of XAFS

structural signal:

χ

(k)

Structural

refinement

Check the results

END

Preliminary

data treatment

Structural

model(s)

re vi si on re vi si on revision
(22)

Preliminary data treatment &

Extraction of XAFS structural signal:

χ

(k)

List of files (group) opened into Athena

Plot highlighted files

Plot (several) marked files

Options for plot

Warning: check if the full windows is visible on your PC,

smal screens (i.e. e-pc) may cut the lower part

Warning: check the graphic windows and never close it

leaving Athena/Artemis open… sometime the PC

(23)

Open

cu_foil_10k.dat

into Athena

Example 1: Cu 10 K

Exercise 1: Look at the results obtained using the automatic extraction playing with plot options

(24)

Takes the value from the

cursor on the graph window

Exercise 2: Look at the effects

of changing background

subtraction parameters

R cut off for automatic background calculation - Change Eo - Change Rbkg - ....

Rbkg = 0.2

Rbkg = 1

Rbkg = 2

Select Eo

Cut off structural information !!!!

(25)

Exercise 3: in Real space look at

the effects of changing extraction

and FT parameters

FT of: kkwχ (k)

R- space

K- space

(26)

Exercise 4: in q (Back Fourier) space

look at the effects of changing BF

(27)

Exercise 5: Data treatment

Shifts the spectrum to have selected point (reference at) at the calibration energy

(calibrate to)

Experimental data

(28)

Save:

cu_foil_10k.dat.chi

χ(k) is required for ARTEMIS

Note: Arthemis requires

equispaced k data !!! (i.e. δk = 0.05)

You cannot use

χχχχdata if not equispaced

(29)

Working with several files

Go into the

Fe_Align

directory

Open all

Fe files

into Athena

Fe 60 K, scan 1 Fe 60 K, scan 2 Fe 60 K, scan 3 Fe 300 K, scan 2 Fe 300 K, scan 1 Fe 150 K, scan 1

(30)

Exercise 6: align Eo

Open

Fe files

into Athena

Eo is shifted among the files !!!

(31)

Exercise 7: Merge several files

Fe 60 are now aligned

(32)

Full Exercise:

1. Read Fe Files

2. Align Fe files on order to have the same Eo

3. Merge files having the same T

4. Save

χ

(k) of merged files, to be used for the

structural analysis

(33)

Structural model & Data refinement

Cu-fcc metal SPG: fcc, f m 3 m (# 220) a = 3.61 A Cu 0.0 0.0 0.0 I II III V IV Sh R N RCu(A) I: a/sqrt(2) 12 2.553 II: a 6 3.610 III: a.sqrt(1.5) 24 4.421 IV: a.sqrt(2) 12 5.105 V: a.sqrt(2.5) 24 5.708 .... icsd_43493_Copper.cif
(34)

Depends on what is highlighted in the Data & Paths panel

Structural model & Data refinement

Start the ARTEMIS program

Controls for plotting

Start the refinement

Warning: check the full windows is visible on

your PC, smaller screens may cut the

lower part The ARTEMIS panel

Warning: check the graphic windows and never close it leaving Athena/Artemis open…

sometime the PC crashes

(35)

Structural model & Data refinement

Theory

new atoms page

- Import Cu.inpfile from the Cu_10kdirectory Or

- Blank Atom page (you must type the crystallographic info)

Warning: check the full windows is visible on

your PC, smaller screens may cut the

(36)

Sh R N RCu(A) I: a/sqrt(2) 12 2.553 II: a 6 3.610 III: a.sqrt(1.5) 24 4.421 IV: a.sqrt(2) 12 5.105 V: a.sqrt(2.5) 24 5.708 .... 1 3 2 4 5 Define the parameters describing the structure

Check the distances and multiplicities are those you expect

(37)

1

2

3

(38)

Open Cu_foil_10k.inp

Using CRTL key you can select groups for plot

(39)

1

st

shell analysis

Right click

remove all paths or

restart ARTEMIS

add 1st shell path to the list

(40)

Path label So2

Energy shift Distance correction

Debye Waller factor

guess: optimized in the refinement

def: math expressions updated during the fit

set: numbers or expressions evaluated once at the fit beginning and not updated

The Data screen allow defining the fitting strategy and

(41)

ν = Nind-Nvar

Absolute misfit between experimental data and theory The refinement is performed in Real space, on the

(42)

Structural results

ri gh t cl ic k
(43)

Effects of Fitting parameters

Kwt = 1

(44)

Single Scattering

MS + Focusing

Add new contributions

I II III V IV SS MS 3-legs MS 3-legs MS 4-legs Visualize the structure and understand the neighbour shells! Take care about multiple scattering contributions

(45)

1 4 1 4 + 1 4 + 1 1 4 + 1 4 + MS paths + SS paths

Understand the MS contributions!!!

Focusing effect may

raises some MS

contributions well above

the SS one

(46)

In principle different for each shell

In principle the same for each shell

Warning:

The used path must be inside the fit range

(47)
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(49)
(50)
(51)

it's your work now!

a. Fe bcc

b. GeO

c. ...

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