Brief X ray powder
diffraction analysis tutorial
•
•
Bibliografia essenziale
Bibliografia essenziale
•
•
X
X
-
-
ray powder diffraction (XRPD): un
ray powder diffraction (XRPD): un
breve
breve
richiamo
richiamo
•
•
Analisi qualitativa
Analisi qualitativa
•
•
Analisi
Analisi
quantitativa
quantitativa
(
(
metodo
metodo
Rietveld)
Rietveld)
Dr Carlo
Dr Carlo
Meneghini
Meneghini
Dip. Di Fisica, Università di Roma Tre
[email protected]
Bibliografia essenziale
Pwder diffraction: technique and data analysis
• B.E. Warren, X-Ray Diffraction (Addison-Wesley, 1990).
• H.P. Klug and L.E. Alexander, X-Ray Diffraction Procedures (Wiley Interscience, 1974). • B.D. Cullity, Elements of X-Ray Diffraction (Wiley, 1978).
• Modern Powder Diffraction Reviews in Mineralogy, Volume 20 D.L. Bish and J.E. Post, Editors Mineralogical Society of America, 1989.
• Fundamentals of Crystallography IUCr Texts on Crystallography -2 C. Giacovazzo, Editor Oxford Science Publication, 1992.
• The Rietveld Method IUCr Monographs on Crystallography - 5 R.A. Young, Editor Oxford Science Publication, 1993.
• X-ray Diffraction Procedures for Polycrystalline and Amorphous Materials H.P Klug and L.E. Alexander Wiley-Interscience, 1974, 2nd edition.
• Defects and Microstructure Analysis by Diffraction R.L. Snyder, J. Fiala and H.J. Bunge, IUCr Monographs on Crystallography, Vol 10, Oxford Science Publications, 1999.
On line resources
http://epswww.unm.edu/xrd/resources.htm
http://www.ccp14.ac.uk/
10
20
30
40
2θ
Atomic
distribution in
the unit cell
Peak relative
intensities
Unit cell
Symmetry
and size
Peak
positions
a
b
Peak shapes
Particle size
and defects
Background
Diffuse scattering,
sample holder,
matrix, amorphous
phases, etc...
X-ray Powder Diffraction
NOTA
Determinare una struttura cristallografica ab-initio
(metodi diretti) da misure XRPD è cosa molto difficile,
complessa e delicata
**
.
Piú normale è "raffinare" le informazioni strutturali a
partire da modelli, ipotesi e conoscenze a-priori sul
campione.
**
Structure determination from Powder diffraction data
•Harris, K.D.M., M. Tremayne, and M. Kariuki. Contemporary Advances in the Use of Powder X-Ray Diffraction for Structure Determination, Angew. Chem. Int. Ed. 40 (2001) 1626-1651.
•Giacovazzo, C. Direct Methods and Powder Data: State of the Art and Perspectives, Acta Crystallogr. A52 (1996) 331-339.
•Scardi, P., et al. International Union of Crystallography Commission for Powder Diffraction. http://www.iucr.org/iucr-top/comm/cpd/
Powder diffraction patterns
2d
hkl
sin(2θ) = nλ
Bragg law
Unit cell
Symmetry
and size
1
k
k’
q
d
hkl|k|=|k’|
q=sin(θ) 4πλ
−1 (exchanged momentum vector)Peak intensity
I
hkl
~ |F
hkl
|
2
e
-q
2u
2=
Debye Waller factor
u = mean square displacement u=<r
n-r
o>
Structural Disorder:
f
n
= f
no
e
-q
2u
22b
F
hkl
= structure factor
F
hkl
= Σ f
n
e
ik.r
nAtomic distribution
in the unit cell
2a
Line shape
anisotropy
Crystallite defects
β
τ
=D-d
Crystallite size
Sherrer Law
breath
www.fis.uniroma3.it/~meneghini
analisi dati
SNLS – XRPD tutorial
Programmi
Gnuplot
PCW
GSAS
gp400win32.zip
Analisi
Dati
Y2O3_PCW
Y2O3_GSAS
UTIL
Au_GSAS
www.gnuplot.info
0 5000 10000 15000 20000 25000 0 20 40 60 80 100 120 'y2o3.dat' u 1:2SNLS/dati
plo_y2O3.plt
gnuplot> pl [:][:] 'y2o3.dat' u 1:2 w l
x-range
xrd-file
u
sing
x:y
columns
w
ith
l
ine
Possibili candidati
http://barns.ill.fr
0 5000 10000 15000 20000 25000 10 20 30 40 50 60 'y2o3.dat' u 1:2
y2o3.dat
database
http://database.iem.ac.ru/mincryst/
0 5000 10000 15000 20000 25000 10 20 30 40 50 60 'y2o3.dat' u 1:2y2o3.dat
SNLS – XRPD tutorial
http://users.omskreg.ru/~kolosov/bam/a_v/v_1/powder/details/pcwindex.htm
pcw23.exe
Programmi
Gnuplot
PCW
GSAS
Analisi
Dati
Y2O3_PCW
Y2O3_GSAS
UTIL
Au_GSAS
icsd_86815.cel
y2o3.x_y
diffracted
beam
incoming
beam
θ
y2o3.x_y
y2o3.x_y
Rietveld method
I
calc
= I
bck
+ S
Σ
hkl
C
hkl
(θ)
F
2
hkl
(θ)
P
hkl
(θ)
background
Scale
factor
Corrections
Miller
Structure
factor
Profile
function
Structure
Structure
Symmetry
Symmetry
Experimental
Experimental
Geometry
Geometry
set
set
-
-
up
up
Atomic positions,
Atomic positions,
site occupancy
site occupancy
& thermal
& thermal
factors
factors
particle size,
particle size,
stress
stress
-
-
strain,
strain,
texture
texture
+
+
Experimental
Experimental
resolution
resolution
Sample
diffracted
beam
incoming
beam
2θ
displacement zeroshiftI
calc
= I
bck
+ S
Σ
hkl
C
hkl
(θ)
F
2
Refinement of y2o3.x_y 12/10/2005 12.58.11
¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯
R-values Rp=18.08 Rwp=24.85 Rexp=2.01 2 iterations of 6
parameter old new icsd_86815 ¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯ scaling : 1.2000 1.2000 lattice a : 10.5968 10.6090 profile U : -0.1870 -0.4973 PsVoigt2 V : 0.0020 0.7986 W : 0.1050 -0.2679 overall B : 0.0000 -global parameters ¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯¯ zero shift : -0.1475 -0.1997 displacement : 0.0000 -backgr. polynom : 13 13 coeff. a0 : 4515.8630 6590.1070 a1 : -841.4 -1060 a2 : 68.74 75.86 a3 : -2.669 -2.745 a4 : 0.05247 0.0522 a5 : -0.0004457 -0.0004386 a6 : -6.29E-7 -5.966E-7 a7 : 3.161E-8 3.121E-8 a8 : -3.797E-12 -8.06E-12 a9 : -1.953E-12 -1.947E-12 a10 : 2.97E-16 6.361E-1 a11 : 1.251E-16 1.261E-1 a12 : -6.315E-19 -6.571E-1 a13 : 8.173E-22 8.861E-2
GSAS
GSAS
SNLS – XRPD tutorial
(XP)gsas+expgui.exe
Programmi
Gnuplot
PCW
GSAS
Analisi
Dati
Y2O3_PCW
Y2O3_GSAS
UTIL
c:\gsas\mywork
Au_GSAS
y2o3.
y2o3.
gs
gs
,
,
y2o3.
y2o3.
exp
exp
,
,
inst
inst
_
_
xry
xry
.
.
prm
prm
http://www.ccp14.ac.uk/solution/gsas/gsas_with_expgui_install.html
Obtaining GSAS
I
calc
= I
bck
+ S
Σ
hkl
C
hkl
(θ)
F
2
peak variance:
peak variance:
σ
2=
GU
tan
2θ
+
GV
tan θ +
GW
tan
2q +
GP
/cos
2θ
sample shift:
sample shift:
s = - π R
shft
shft
/ 3600
sample absorption:
sample absorption:
µ
eff= - 9000 / (π R
Asym
)
Gaussian Sherrer broadening
Lorentzian
Lorentzian
:
:
γ
= (
LX
LX
-
ptec
ptec
cos φ)/cos θ + (
LY
LY
-
stec
stec
cos φ) tan θ
Anisotropy Lorentzian strain broadening Anisotropy (stacking faults) Lorentzian Sherrer broadening (particle size)
peak variance:
peak variance:
σ
2=
GU
tan
2θ
+
GV
tan θ +
GW
tan
2q +
GP
/cos
2θ
Lorentzian
Lorentzian
:
:
γ
= (
LX
LX
-
ptec
ptec
cos φ)/cos θ + (
LY
LY
-
stec
stec
cos φ) tan θ
Strain:
S
= ∆d/d
Gaussian contrib.
S
= sqrt[8 ln 2 (
GU
-
U
i)] (π/18000) · 100%
Instrumental
contribution
Lorentzian contrib.
S
= (
LY
–
Y
i) (π/18000) · 100%
Instrumental
contribution
Particle size:
P
P = (18000/ π) K
λ
/
LX
Scherrer
constant
1
2
3
Mp =
Σ
w (I
exp-I
calc)
2Rp =
Σ
(I
exp-I
calc) /
Σ
I
expwRp = sqrt[ Mp /
Σ
I
2exp