Linda Lim Stanford University Stanford Synchrotron ... · Structure Refinement Linda Lim Stanford...

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Structure Refinement Linda Lim Stanford University Stanford Synchrotron Radiation Lightsource Stephens’ Law – “A Rietveld refinement is never perfected, merely abandoned” Demonstration: Rietveld Refinement of spinel oxide

Transcript of Linda Lim Stanford University Stanford Synchrotron ... · Structure Refinement Linda Lim Stanford...

Page 1: Linda Lim Stanford University Stanford Synchrotron ... · Structure Refinement Linda Lim Stanford University Stanford Synchrotron Radiation Lightsource Stephens’ Law – “A Rietveld

Structure Refinement

Linda Lim

Stanford University

Stanford Synchrotron Radiation Lightsource

Stephens’ Law –“A Rietveld refinement is never perfected,

merely abandoned”

Demonstration: Rietveld Refinement of spinel oxide

Page 2: Linda Lim Stanford University Stanford Synchrotron ... · Structure Refinement Linda Lim Stanford University Stanford Synchrotron Radiation Lightsource Stephens’ Law – “A Rietveld

Outline

List of programs for Rietveld refinement

Rietveld refinement using GSAS

Fourier method

Summary

References

Page 3: Linda Lim Stanford University Stanford Synchrotron ... · Structure Refinement Linda Lim Stanford University Stanford Synchrotron Radiation Lightsource Stephens’ Law – “A Rietveld

Selected list of Programs

o CCP14 for a more complete list(http://sdpd.univ-lemans.fr/du-sdpd/nexus/ccp14/web/index3.htm)

GSAS

GSAS-II

Fullprof

DBW

MAUD

Topas from Bruker – not free

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Example: MnGa2O4

General purpose: to refine a crystal structure

Specific to this example:

Purpose: to find out the site occupancies of

Mn2+ and Ga3+ in octahedral (oct) and

tetrahedral (tet) sites respectively

Why is it significant?

Anti-site defects may affect conductivity due

to generation/compensation of charges

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Page 6: Linda Lim Stanford University Stanford Synchrotron ... · Structure Refinement Linda Lim Stanford University Stanford Synchrotron Radiation Lightsource Stephens’ Law – “A Rietveld

Inverse Modeling Method 1

Rietveld Method

Data

ModelRefined Structure

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nsity

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shape

Background

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1. Model

Sample: MnGa2O4

Spinel AB2O4

Lattice parameter: 8.450 Å

Space group: F d -3 m

Some options:

- Retrieve crystallographic information from powder diffraction database (.cif file)

- Key in the above information directly into

GSAS

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Page 9: Linda Lim Stanford University Stanford Synchrotron ... · Structure Refinement Linda Lim Stanford University Stanford Synchrotron Radiation Lightsource Stephens’ Law – “A Rietveld
Page 10: Linda Lim Stanford University Stanford Synchrotron ... · Structure Refinement Linda Lim Stanford University Stanford Synchrotron Radiation Lightsource Stephens’ Law – “A Rietveld
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Fractional coordinates

- Relative position of a specific atom in the

unit cell

Multiplicity

- How many of a specific atom in the unit cell

UISO

- Isotropic thermal parameter

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2. Profile Shape

From instrument parameter file

Obtain from refinement of calibrant (eg.

LaB6)

Gives the initial values for the profile function

(instrumental only parameters)

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Add screenshot for previous slide on how to load data

and instrument parameter file

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Powpref genles

Run genles until convergence is achieved

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liveplot

First fit!

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3. Background

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3. Background Choose a suitable background function, then refine

background (powpref genles)

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Background has improved

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Lstview

Chi-squared value = 253.5

Shows the

output of the

refined

parameters

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Refine: Scale

Powpref

genles liveplot

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Refine: Scale

Fit has improved!

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Refine: Scale

Chi-squared value = 13.59

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Refine: diffractometer zero

correction

Powpref

genles liveplot

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Refine: Zero

Chi-squared value = 5.543

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Refine: Scale

Chi-squared value = 13.59

Before refining zero

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Refine: cell

Powpref

genles liveplot

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Refine: cell

Chi-squared value = 5.076

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Refine: profile

Peak shapes

K. Stone

Thursday afternoon

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Refine: profile

Chi-squared value = 4.944

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Progress so far

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Inverse Modeling Method 2

Fourier MethodData

ModelRefined Structure

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nsity

Profile

shape

Background

subtract

phases

Integrated

Intensities

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Fourier Difference Map

z

x

y

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Add constraints

Now, we’re adding Mn in octahedral site

and Ga in tetrahedral site

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Add constraintsWe want to see the occupancy of Mn in

octahedral site

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Refine site occupancy

Fix site occupancies after each refinement

F= site occupancy

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Refine fractional coordinates and thermal parameterConstrain x,y,z,u for Td and Oct sites

respectively.

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Refine fractional coordinates and thermal parameter

X= fractional coordinates

U = thermal parameter

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Final Parameters

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Chi-squared value = 2.835Rp = 0.0382

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Fourier difference map

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Summary of refinement

parameters Final site occupancies

Final formula

(Mn0.76Ga0.24)tet (Mn0.21Ga1.79)octO3.9

Anti-site defects are present

Atom Site Occupancy

Mn Tet 0.7573

Ga Tet 0.2427

Mn Oct 0.1064

Ga Oct 0.8963

O 0.9742

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How do you know when to

stop?

Chi-square, liveplot, R factor look good

Most importantly, it has answered the

scientific question you have

Stephens’ Law –“A Rietveld refinement is never perfected,

merely abandoned”

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References

Collaborative Computation Project 14: http://sdpd.univ-lemans.fr/du-sdpd/nexus/ccp14/web/index3.htm

Rietveld mailing list: http://lachlan.bluehaze.com.au/stxnews/riet/using.htm

Brian Toby’s EXPGUI mailing list: http://www.aps.anl.gov/mailman/listinfo/expgui

To download EXPGUI and GSAS as a package: https://subversion.xor.aps.anl.gov/trac/EXPGUI

Powder Diffraction: Theory and Practice (RSC Publishings)

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Acknowledgments

Oak Ridge National Laboratory SNS

US Department of Energy

Page 45: Linda Lim Stanford University Stanford Synchrotron ... · Structure Refinement Linda Lim Stanford University Stanford Synchrotron Radiation Lightsource Stephens’ Law – “A Rietveld

Thank You