in-situ pair distribution function measurements...chapman, chupas, maxey, richardson chem. commun....
TRANSCRIPT
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In-Situ Pair Distribution Function Measurements
Peter J. Chupas
Chemistry, Environmental, and Polymer Science Group
X-ray Science DivisionArgonne National Laboratory
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Talk Overview
(1) PDF Instrumentation (at the APS)
(2) ”Time Resolved” Measurements
(3) Measurements requiring high sensitivity (e.g.. seeing hydrogen with X-rays)
(4) New applications
(5) Potential instrumental developments
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A brief history of X-ray PDF analysis
1930 1940 1950 1960 1970 1980 1990 2000
Computers
1st PD
F
Dire
ct
met
hods
Riet
veld
met
hods
Synchrotrons &Spallation Sources
RE Franklin Acta. Cryst. (1950)
Graphitic Carbon
Tarasov & Warren J.Chem.Phys.(1936)
Liquid Na
RD Shannon J.Phys.Chem.(1985)
Zeolites
HEX+AreaDetectors
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11-ID-B, 11-ID-C
1-ID
6-ID
13-ID
5-BM-D
High Energy X-rays at the APS
Dedicated HEX facilities:1-ID, 11-ID-B, 11-ID-C
Dedicated PDF facility:11-ID-B (since 2005-3)
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The Advanced Photon Source - APS
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High Energy X-Rays at beamline 11-ID at the APS
11-IDThree simultaneously operating stations;
11-ID-D Time Dependent11-ID-C High Energy Scattering11-ID-B Dedicated PDF Beamline
2 Undulators2.3 cm device used by 11-ID-B and -C3.3 cm device utilized by 11-ID-D
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Overview of 11-ID at the APS
11-ID-B
11-ID-C11-ID-D
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High Energy X-rays at the APS
Available Photon Energies:57KeV (Si311)89KeV (Si 511), 120KeV (Si 711), Monochromator: Laue crystal (Fixed Bragg Angle: 3.8o)Max beam size: 3 x 2 mm2
Flux: 1012 Photons/s
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Dedicated PDF facility at the APS
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The Pair Distribution Function Method
0 10 20 30Q
Inte
nsity
Measured Diffraction Intensity
0 2 4 6 8 10
G(r) = 4πr[ρ(r)-ρ0]
G(r)G(r
)/ Å
-2
r / Å
Si-O 1.6Å
O…O 2.6Å
Si…Si 3.2Å
I(Q) S(Q)
=4πsinθ/λ
FourierTransform
– The structure factor S(Q) can be measured as a function of diffraction angle using monochromatic X-rays
– Application of area detector to yield more rapid measurements by collecting all data simultaneously
P.J. Chupas, X. Qiu, J.C. Hanson, P.L. Lee, C.P. Grey, S. Billinge, J. Applied Cryst., 2003, 36, 1342-1347.
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High Real Space Resolution PDFs:The Need for High Q Measurements
2 4 6 8 10 12 14r(Å)
Qmax = 10 Å-1
Qmax = 15 Å-1
Qmax = 20 Å-1
Qmax = 25 Å-1
2 4 6 8 10 12 14r(Å)
Qmax = 10 Å-1
Qmax = 15 Å-1
Qmax = 20 Å-1
Qmax = 25 Å-1
Qmax=4πsinθ/λ
for Cu Kα, λ=1.54Å, 2θ=180o
Qmax = 4πsin90/1.54 = 8 Å-1
We typically use wavelengths between 0.20 and 0.08 Å
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Accessibility to high resolution measurements
•Sample volume ~ 0.08 mm3
•Detector specific corrections are VERY import•Energy sensitivity and Compton Scattering•“Oblique Incidence”
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Refinement Against Crystalline Models
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In situ reduction: PtIVO2 → Pt0
Chupas, Chapman, Lee J. Appl. Crystallogr., 2007, 40, 463-470
Data can be collected in only 30 ms
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In-situ measurements: The reduction of PtO2 to Pt
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Application of Time Resolved Studies:
Supported Metal CatalystsFollowing the kinetics formation of catalytic particles
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TiO2 Substrate
H2/200oC 200oC
Forming Supported Nanoparticles
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Pt4+ + 4 e- → Pt0
H2 → 2H+ + 2e-
Forming Supported Nanoparticles
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Gas in Gas out
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Reduction of 5% Pt4+ on TiO2 Under H2
•Reduction at constant temperature, 200 ˚C
Ti-O
O-OPt-Pt
5wt % Pt on TiO2(via aqueous impregnation with H2PtCl6)
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In situ reduction: Pt4+ on TiO2 → Pt0
H2
1-ID-C
Chupas, Chapman, Jennings, Lee, Grey J. Am. Chem. Soc., in press
G(r)Pt/TiO2− G(r)TiO2
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Tracking the Kinetics of Particle Formation
Pt-Cl correlation
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Tracking the Kinetics of Particle Formation
Pt-Cl correlation
zero-order reactionr = k
The rate is independent of concentration for a zero-order reaction.
Zero-order reactions can be found when a material required for a reaction to proceed (such as a surface) is saturated by the reactants
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Nest Step: Particle Growth
Pt-Pt correlation
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Combined PDF and SAXS measurements
e− orbition
chamber
sampledouble crystal
monochromatorslits
area detector
beam stop
area detector
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Overview
Differential PDF selectively probes supported nanoparticles– Fast time resolution possible– Follow reaction
Probes reaction mechanism & kinetics– Reagent consumption (bonds breaking) – Bond formation– Particle growth/annealing
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Can we probe the structure of weakly bound guest molecules?
Are open metal sites important for binding H2?
Seeing hydrogen with X-rays?!
Porous Coordination Frameworks
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Open Metal Sites in Prussian Blue Analogues
e.g. MnII
3[CoIII(CN)6]2
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Open Metal Sites in Prussian Blue Analogues
e.g. MnII
3[CoIII(CN)6]2
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Open Metal Sites in Prussian Blue Analogues
e.g. MnII
3[CoIII(CN)6]2
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Open Metal Sites in Prussian Blue Analogues
e.g. MnII
3[CoIII(CN)6]2
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-0.3%
-0.2%
-0.1%
0.0%
0.1%
0.2%
0.3%
50 100 150 200 250 300 350 400
Temperature/K
Rel
ativ
e C
hang
e in
Lat
tice
Para
met
er
MnII3[CoIII(CN)6]2
Prussian Blue
N2 Sorption
N2
Under He
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Differential PDF
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Differential PDF
Chapman, Chupas, Kepert J. Am. Chem. Soc. 127, 2005, 11232-11233
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Differential PDF
N-N distance in N2 moleculeChapman, Chupas, Kepert J. Am. Chem. Soc. 127, 2005, 11232-11233
11-ID-B
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Differential PDF
N-framework & N-N interactionsChapman, Chupas, Kepert J. Am. Chem. Soc. 127, 2005, 11232-11233
11-ID-B
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Differential PDF
Chapman, Chupas, Kepert J. Am. Chem. Soc. 127, 2005, 11232-11233
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Hydrogen Differential PDF
H2-framework interactionsChapman, Chupas, Maxey, Richardson Chem. Commun. 2006, 4013-4016
Contribution from disordered H2evident from
X-ray scattering
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Structural Models
Binding at open metal sites
van der Waals interactions only
Chapman, Chupas, Maxey, Richardson Chem. Commun. 2006, 4013-4016
11-ID-B
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GPPD, IPNSStructural Models
Binding at open metal sites
van der Waals interactions only
Chapman, Chupas, Maxey, Richardson Chem. Commun. 2006, 4013-4016
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Enhancing Sorption
Smaller Pores
GreaterΔ
Hsorption
Tune compositionie. pore size M3[Co(CN)6]2
Chapman, Chupas, Maxey, Richardson Chem. Commun. 2006, 4013-4016
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Applications of Micro-focused High-Energy X-rays(available at 1-ID at the APS)
-High pressure Studies from Diamond Anvil Cells
-Spatially Resolved Measurements
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Bent Laue MonochromatorFocusing Lens
(Si saw-tooth type*)
Focusing High-Energy X-Rays at 1-ID
*S. D. Shastri et al., J. Synchrotron Rad., 14, 204 (2007)
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PDF at High Pressures
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PDF of Gold in the DAC and Measured ex-situ
Martin, Antao, Chupas, Lee, Shastri, Parise Applied Physics Letters 86 (2005) 061910.
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High Pressure PDF
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Gold at High Pressures
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Looking Ahead:The Potential for Future Instrumentation Developments
-Rapid Energy Resolved Measurements
-Simultaneous Measurements (e.g. combining PDF with SAXS)
-Anomalous
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Petkov, Billinge, Shastri, Himmel, Phys Rev. Lett. 85, 3436 (2000)
Compton Scattering
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Common Instrumentation Configurations
e− orbit
double crystalmonochromator
ionchamber
slitssample
diffractometer
analysercrystal
detector
e− orbit
double crystalmonochromator
ionchamber
slitssample
area detector
beam stop
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Rapid Energy Resolved Measurements?
Beno and Knapp Review of Scientific Instruments (1995) 60, 1308-1310.
Cs2Ge4O9
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High Energy Resolution Optics for High-Energy X-rays:
Potential for Anomalous PDF Measurements
S. D. Shastri, J. Synchrotron Rad., 11, 150 (2004)
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Example of High-Energy Resonant Scattering
Ion Distribution in Pb5Bi6Se14
Bi and Pb distributed over 11 crystallographically unique sites
Zhang, Wilkinson, Lee, Shastri, Shu, Chung, Kanatzidis, J. Applied Crystall., 38, 433 (2005)
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AcknowledgementsKarena W. Chapman (XSD, ANL)
Evan R. Maxey (XSD, ANL)James Richardson (IPNS, ANL)
Peter L. Lee (XSD, ANL)Guy Jennings (XSD, ANL)
Mark Beno (XSD, ANL)Sarvjit Shastri (XSD-ANL)
Clare P. Grey (Stony Brook)John B. Parise (Stony Brook)C. David Martin (XSD, ANL)Gabrielle Long (XSD, ANL)
John W. Cahn (NIST)Leo Bendersky (NIST)Simon Billinge (MSU)Xiangyun Qiu (MSU)
Work performed at the Advanced Photon Source was supported by the U.S. Department of Energy, Office of Science, Basic Energy Sciences, under Contract No. DE-AC02-06CH11357.