synchrotron radiation for material analysis
DESCRIPTION
Synchrotron Radiation for Material Analysis. M. Aslam Baig National Center for Physics Quaid- i - Azam University Campus, Islamabad Pakistan [email protected] [email protected]. K . Vacuum tube. Characteristic radiation. Anode. Intensity (a. u.). X-rays. Bremsstrahlung radiation. - PowerPoint PPT PresentationTRANSCRIPT
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M. Aslam BaigNational Center for Physics
Quaid-i-Azam University Campus, IslamabadPakistan
[email protected] [email protected]
Synchrotron Radiation for Material Analysis
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X-ray ray tubes
0.02 0.04 0.06 0.08 0.10Wavelength (nm)
Inte
nsity
(a.
u.)
K
K
min
Characteristicradiation
Bremsstrahlungradiation
The spectrum from an X-ray tube has discrete fluorescent lines superimposed on the continuous bremsstrahlung radiation
Anode
Vacuum tube
CathodeElectrons
HV
Filament supply
X-rays
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Energy Dissipation
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BAIG, Karachi, 7th. January, 2005
How a Storage Ring Works
Electrons aregenerated here
And initiallyaccelerated inthe LINAC
How does it work?
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Radiation angular distribution (a) electrons travelling at low speed(b) electrons travelling at relativistic speed (g = (1-v2/c2)-1/2 10000 at ESRF)
Synchrotron radiation angular distribution
Electron orbit
Acceleration
v << c
v c
Electron orbit
Acceleratione-
e-
Q m0c2/E= 1/g radm0 = electron mass
v = electron velocityE = electron energyc = velocity of light
v
v
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Time structure
t
I
1ms
100 ps
e- e-e-e-
Time pulsed emission is interesting for studying rapid reactions
Light pulses
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Als-Nielsen Introduction to Modern X-ray Physics
Synchrotron storage ring
Spectrometer
Monochromator Undulator
300 m
Focusing device
10 m
2 m30 m
From the magnetic device to the experimental station
5 m
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Why is wavelength important?
Why is it special?
Visible light X-rays
To penetrate a sample, you need a wavelength of similar, or smaller magnitude.
sample sample
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DetectorSampleX-rays
Absorption
X-rays
Sample
I
wavelength
Fluorescence
Imaging
DetectorX-rays
Elemental analysis
88000.0
8800 9000 9200 9400 9600 9800 10000
1.0
2.0
E (eV)9000 9200 9400 9600 9800 10000
Energy
m
Detector
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The absorption coefficient μ
t
I = I0 exp(-μt)
linear absorption coefficient
α = μt = ln ( I0/I )
I0 I
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9.4 9.6 9.8 10.0 10.2 10.4 10.60.5
1.0
1.5
2.0
2.5
3.0
mt
(E) (a
rb. u
nits.)
Energy (keV)
X-rayAbsorptionFine Structure
Zinc K-edge
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Extended X-ray absorption fine structure (EXAFS)
In condensed matter the ejected photo-electron (wave) will be scattered by neighbouring atoms. It is the interference between the outgoing electron and the back-scattered ones which leads to oscillations visible in the absorption spectrum above the edge.
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Extended X-ray absorption fine structure (EXAFS)
Lab data took over 12 hours to collect.
Synchrotron data took 25 minutes and could have been collected in about 3.
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Taken from:“Introduction to Powder Diffraction”By: R J CernikDaresbury Laboratory
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Powder Diffraction
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XANES can be used simply as a fingerprint of phases and oxidation state.
Fe compounds
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FLASH – Light Source
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Photoionization of Neon
Richter et al PRL 102, 163002, 2009
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Xenon Ions
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Bi1.7 Pb0.4 Sr2 Ca2 Cu2 O4
0 100 200 300
0.0
3.0
6.0
CaO
SrCaO2
Cu2O
Pb/Bi
Ca2CuO3
Sr
SrO
Ca
Mg
Mass / charge (m/q)
Rel
. Sig
nal I
nten
sity
(arb
. uni
ts)
Surface analysis of superconducting materials
Baig et al J.Appl. Phys. 2009
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Future…….
• Prospects for Pakistan
SESAME • Synchrotron Radiation Facility being built in
Amman, Jordan