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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]

(2)

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/

(3)

10

20

30

40

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

(4)

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/

(5)

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

2

u

2

=

Debye Waller factor

u = mean square displacement u=<r

n

-r

o

>

Structural Disorder:

f

n

= f

no

e

-q

2

u

2

2b

F

hkl

= structure factor

F

hkl

= Σ f

n

e

ik.r

n

Atomic distribution

in the unit cell

2a

(6)

Line shape

anisotropy

Crystallite defects

β

τ

=D-d

Crystallite size

Sherrer Law

breath

(7)

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

(8)

www.gnuplot.info

0 5000 10000 15000 20000 25000 0 20 40 60 80 100 120 'y2o3.dat' u 1:2

SNLS/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

(9)

Possibili candidati

http://barns.ill.fr

(10)

0 5000 10000 15000 20000 25000 10 20 30 40 50 60 'y2o3.dat' u 1:2

y2o3.dat

database

(11)

http://database.iem.ac.ru/mincryst/

0 5000 10000 15000 20000 25000 10 20 30 40 50 60 'y2o3.dat' u 1:2

y2o3.dat

(12)
(13)

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

(14)
(15)

diffracted

beam

incoming

beam

θ

(16)

y2o3.x_y

y2o3.x_y

(17)

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

(18)

Sample

diffracted

beam

incoming

beam

displacement zeroshift

(19)

I

calc

= I

bck

+ S

Σ

hkl

C

hkl

(θ)

F

2

(20)
(21)

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

(22)

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

(23)
(24)

I

calc

= I

bck

+ S

Σ

hkl

C

hkl

(θ)

F

2

(25)

peak variance:

peak variance:

σ

2

=

GU

tan

2

θ

+

GV

tan θ +

GW

tan

2

q +

GP

/cos

2

θ

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)

(26)

peak variance:

peak variance:

σ

2

=

GU

tan

2

θ

+

GV

tan θ +

GW

tan

2

q +

GP

/cos

2

θ

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

(27)

1

2

3

Mp =

Σ

w (I

exp

-I

calc

)

2

Rp =

Σ

(I

exp

-I

calc

) /

Σ

I

exp

wRp = sqrt[ Mp /

Σ

I

2

exp

]

χ

2

= Mp / (N

(28)

GSAS

GSAS

SNLS – XRPD tutorial

(XP)gsas+expgui.exe

Programmi

Gnuplot

PCW

GSAS

Analisi

Dati

Y2O3_PCW

Y2O3_GSAS

UTIL

Au_GSAS

c:\gsas\mywork

(29)

GOLD

S

F m3m

λ=0.688011

Au= 0. 0. 0.

a = 4.0782

References

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