Oxide Formation of Transition Metal Surfaces and Effect on … · 2015. 5. 7. · Oxide Formation...
Transcript of Oxide Formation of Transition Metal Surfaces and Effect on … · 2015. 5. 7. · Oxide Formation...
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Wei-Xue Li
State Key Laboratory of Catalysis, and Center for Theoretical and Computational Chemistry
Dalian Institute of Chemical Physics, China
Oxide Formation of Transition Metal Surfaces and Effect on Catalysis
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H. Over et al, Science 287, 1474 (2000)
CO Oxidation on Ru(0001) versus RuO2(110)Langmuir-Hinshelwood versus Mars-Van Krevelen
RuO2 Ru(0001)
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J. Gustafson et al, PRL (2004)
C.I.Carlisle et al, PRL (2000)
E. Lundgren et al, PRL (2002)
Ag(111)A zoo of
surface oxide
Rh(111) Surface oxide (metal stable)
Pd(111)Surface oxide
H. Over et al, Science (2000)
Ru(0001) bulk oxide
Sc Ti V CrMn Fe Co Ni Cu Zn
Y Zr NbMo Tc Ru Rh Pd Ag Cd
La Hf Ta W Re Os Ir Pt AuHg
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Pressures and Materials Gap
Working Conditions: Working Conditions: atmospheric pressures and elevated temperatures atmospheric pressures and elevated temperatures
Surface Science: Ultra high vacuum / single crystal
Role of the atmospheric environment, i.e. species and gas pressure, as well as the temperature, need to be considered !
``Material-gap’’``Pressure-gap’’ (1012 magnitude difference)
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Apparatus
Density Density ffunctional unctional ttheory heory (DACAPO, FHIMD)(DACAPO, FHIMD)Plane Wave Basis Set, GGA, USPP, SlabPlane Wave Basis Set, GGA, USPP, Slab
Transition State TheoryTransition State TheoryAb initio ThermodynamicsAb initio ThermodynamicsKinetic Monte CarloKinetic Monte Carlo
Microscopy (HPMicroscopy (HP--STM, TEM)STM, TEM)Synchrotron (XPS, HPSynchrotron (XPS, HP--SXRD)SXRD)Vibration Spectroscopy (HREELS)Vibration Spectroscopy (HREELS)etcetc
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Oxidation of Ag(111) and ethylene epoxidationOxidation of Pt(332) and CO OxidationOxidation of Pt(110) and CO OxidationOxidation of Rh(110) and H2 Reduction
Sc Ti V Cr Mn Fe Co Ni Cu Zn
Y Zr Nb Mo Tc Ru Rh Pd Ag Cd
La Hf Ta W Re Os Ir Pt Au Hg
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Silver is unique catalyst foroxidation of ethylene to epoxide (P=1atm, T=500-600K)
CC22HH44++11//22OO22 CC22HH44OO,
partial oxidation of methanol to formaldehyde (P=1atm, T=700-900K)CHCH33OH+ OH+ 11//22OO22 CHCH22O+ HO+ H22O,O,
but silver is noble metal, bind particles only weaklythoughts: bulk dissolved oxygen may be important
O-Ag(111) interaction, looks simple, but big challenging !
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Oα OβOγ
Experimental Results: (TPD)
OγOα
Oβ
O2
Solid
gas
T
T T
(Herein, et al., Zeit. Phys., 1996)Proposed that O speciesProposed that O speciesInterInter--change sites change sites depending on P and Tdepending on P and T
Inte
nsity
(nor
mal
ized
) AlphaBetaGammaConvs.
300 400 500 600 700 800 900Desorption Temperature [K]
Temperature Programmed Desorptionidentifies 3 O species
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Ordered Structures: O/Ag(111)(4x4)(4x4)--OO (Carlisle et al, PRL, 2000)
Schnadt et al, Phys. Rev. Lett. 96, 146101 (2006)
Schmid et al, Phys. Rev. Lett. 96, 146102 (2006)
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Metal substrate
Clean Surface Chemisorption
Surface Oxide Bulk Oxide
O2 gas
Ag(111) surface
Metal substrateAg(111) surface
Metal substrate
O2 gas
Metal substrate
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Oxygen chemisorptions on late 4d transition metals
-Filling of d-band weakens substrate-adsorbate bond
- Repulsive interaction within electronegative adlayer
Todorova, Li, Pirovano, Stampfl, Reuter, Scheffler, Phys. Rev. Lett. 89, 096103 (2002)
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The Role of the O-Ag Interaction in the function of Silver as an Oxidation Catalyst
0 0.2 0.4 0.6 0.8 1 1.2Coverage θ (ML)
2.0
2.4
2.8
3.2
3.6
4.0
Ads
orpt
ion
ener
gy (
eV /a
dato
m)
subsurface-octa.
fcc
ozone-like
oxide-like
bulk-subst.
surface-subst.
bulk-octa.
(4x4)
Li, Stampfl, Scheffler, Phys. Rev. B, 68, 165412 (2003), Phys. Rev. B. 67, 045408 (2003), Phys. Rev. B, 65, 075407 (2002)
DFT Calculations
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From UHV to Real World (Theoretical Recipes)Ab initio atomistic thermodynamics
),(),(),(),( OxygenMetalMetalOxygen,Metal Oxygen, PTNPTGPTGPTG μ−−=Δ
GO,Metal (T,P): Gibbs free energy after adsorption
Reuter and Scheffler, Phys. Rev. B (2002)Li, Stampfl and Scheffler, Phys. Rev. B 68, 165412 (2003)
Gibbs Formation Energy of Adsorption
Extended System: G(T,P)= Etot + Fvib + pV
Molecule in Gas Phase: μμOO (T,p) = (T,p) = μμOO (T,p(T,p00) + 1/2k) + 1/2kBBT ln (p/pT ln (p/p00))
),()()(),( OxygenMetalMetalOxygen,Metal Oxygen, PTNDFTEDFTEPTG μ−−=Δ
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Average Gibbs free energy of adsorptionAverage Gibbs free energy of adsorptionLi, Stampfl, Scheffler, Phys. Rev. Lett. 90, 256102 (2003)
Michaelide, Reuter and Scheffler, JVST(A) 23, 1487 (2005)
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Pressure – Temperature Phase Diagram: O/Ag(111)bases on ab initio atomistic thermodynamics
Li, Stampfl and Scheffler, Phys. Rev. Lett. 90, 256102 (2003)
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Oxidation of Ag(111) and ethylene epoxidationOxidation of Pt(332) and CO OxidationOxidation of Pt(110) and CO OxidationOxidation of Rh(110) and H2 Reduction
Sc Ti V Cr Mn Fe Co Ni Cu Zn
Y Zr Nb Mo Tc Ru Rh Pd Ag Cd
La Hf Ta W Re Os Ir Pt Au Hg
steps
kinks (335)
(11 13 19)
vicinal surfaces
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T.Zambelli, J. T.Zambelli, J. Wintterlin, J. Trost, Wintterlin, J. Trost,
G. Ertl, Science G. Ertl, Science 273273, 1688 (1996)., 1688 (1996).
NO dissociation at Ru stepsNO dissociation at Ru steps
Ea=1.24 eV Ea=0.20 eV
• High εd’s atsteps.
• More activemetal atoms.
Hammer (1999).
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Oxide Nucleation and Growth of Rh(111) along Step Edge
J. Gustafson et al, PRL 92, 126102 (2004)
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FV
ckin
EEhv−Ε=
++=φ
εφ
hv Binding energy
Vacuum Level, Ev
Fermi Level, EF
φKinetic energy
Core level
X-ray Photoelectron Spectroscopy (XPS)
Element specific and geometric sensitiveFingerprint as adsorption site and oxidation state
Surface Core Level Shift
E(n))E(nεc −−= 1E(n) / E(n-1): total energy before / after core excited (frozen core approximation, valence electron relaxation included)
Core-electron Energy
bulkc
surfcSCLS εε −=Δ
Final state effect included
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Top Bridge
CO Adsorption on Pt(111)
Top
Bridge
DFT Calculations
Wang, Li, Borg, Hammer and Andersen et al. Phys. Rev. Lett. 95, 256102 (2005)
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CO Adsorption on Pt(332)
Wang, Li, Borg, Hammer and Andersen et al. Phys. Rev. Lett. 95, 256102 (2005)
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T. M. Pedersen, J. G. Wang, W. X. Li,and B. Hammer, unpublished
Interaction between oxygen and Pt(332)
per (1x2) cell
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Oxygen coverage varies from 0.37 ML to 0.46 ML without/with oxygen at terrace, which agrees with experimental 0.42 ML results
Calculated Pt 4f binding energy of step Pt atoms coordinated with 4O oxygen atoms agree with experimental finding
O1s binding energy for 4O (step edge) is lower 0.25 eV than 1O (terrace oxygen), which agrees with experimental findings 0.20 eV
Pt(332)
Pt(111)
1D PtO2 along Step Edge of Pt(332)
Wang, Li, Borg, Hammer and Andersen et al. Phys. Rev. Lett. 95, 256102 (2005)
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CO Oxidation on O pre-covered Pt(332)
CO
reaction negligible at 220 K on Pt(332),instead of 270 K on Pt(111)
Wang, Li, Borg, Hammer and Andersen et al. Phys. Rev. Lett. 95, 256102 (2005)
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Wang, Li, Borg, Hammer and Andersen et al. Phys. Rev. Lett. 95, 256102 (2005)
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CO Oxidation on Pt(332)
Reaction Barrier for CO oxidation: 0.60 eV for 1D PtO2 (Eb=0.77 eV for step oxygen)0.71 eV for terrace oxygen (Eb =0.54 eV for terrace oxygen)
Initial State TS
Wang, Li, Borg, Hammer and Andersen et al. Phys. Rev. Lett. 95, 256102 (2005)
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Reactivity of a gas/metal/metal-oxide three-phase boundary
W. X. Li and B. Hammer, Chem. Phys. Lett. (409) 1, 2005
CO Oxidation on oxidized Pt surfaces
Oxidation of Rh(111) SurfaceJ. Gustafson et al, PRL (2004)
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W. X. Li and B. Hammer, Chem. Phys. Lett. (409) 1, 2005
Reactivity at gas/metal/metal oxide three phases boundary
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Enhanced Reactivity at phases boundary
Calculated Barrier for CO OxidationOxide: > 2 eV Metal: 0.78 eVPhases boundary: 0.1-0.65 eV
W. X. Li and B. Hammer, Chem. Phys. Lett. 409, 1 (2005)
Metal Pt(111)
A “Reverse” Model Catalyst
OxideMetal
Oxide PtO2
Phases boundaryp(2x2)-O-CO
c(4x2)-2CO
J. Wintterlin et al, Science 278, 1931 (1997)
Calculated Barrier for CO OxidationInside p(2x2)-O-CO: 0.74 eVPhases boundary: 0.53 eV
Pt(111) Pt(111)-PtO2(0001)
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Oxidation of Ag(111) and ethylene epoxidationOxidation of Pt(332) and CO OxidationOxidation of Pt(110) and CO OxidationOxidation of Rh(110) and H2 Reduction
Sc Ti V Cr Mn Fe Co Ni Cu Zn
Y Zr Nb Mo Tc Ru Rh Pd Ag Cd
La Hf Ta W Re Os Ir Pt Au Hg
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CO oxidation on Pt(110)
B. Hendriksen and J. FrenkenPhys. Rev. Lett. 89, 046104 (2002)
Langmuir Mechanism (metal)Or Mars Van Krevelen Mechanism (Metal Oxide)
C D
STM tip zoom in Reactor
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Helveg, Li, Bartelt, Hammer, Besenbacher et al., submitted to Phys. Rev. Lett.
Low Oxygen Exposure on Pt(110)
T=357 KO dosage up to 205 LFrame rate: 0.12/sec.20.8nm x 22.6 nm
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Oxidation of Pt(110)298K 30x30nm2
500K 6x6nm2 600K 50x50nm2
500K 30x30nm2
Li, Osterlund, Vestergaard, Hammer, Besenbacher et al., Phys. Rev. Lett. 93, 146103 (2004)
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Strained (12x2) Reconstruction
- strained nanostructure (12x2) reconstruction underneathincreased Pt-Pt dist. along [110] (expansion 14 %)2 Pt atoms out of 12 ejected
600K, 4.6x7.7nm2
600K, 50x50nm2
Surface Oxide
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Pederson, Li and Hammer, PCCP 8, 1566 (2006)
0.50 ML 1.00 ML
0.33 ML 0.50 ML 0.67 ML 0.83 ML 1.00 ML
0.92 ML (eV / O atom)
Interaction between oxygen and Pt(110)
Surface Oxide
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T. M. Pederson, W. X. Li and B. Hammer, PCCP 8, 1566 (2006)
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Oxidation of Pt(110)
Li, Osterlund, Vestergaard, Hammer, Besenbacher et al., Phys. Rev. Lett. 93, 146103 (2004)
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(12x2)
Bulk Oxide
Phase Diagram of O/Pt(110) Surfaces
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CO oxidation on Pt(110)
B. Hendriksen and J. FrenkenPhys. Rev. Lett. 89, 046104 (2002)
Langmuir Mechanism (metal)Or Mars Van Krevelen Mechanism (Metal Oxide)
C D
STM tip zoom in Reactor
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Oxidation and Reaction of Pt(110) with CO
T. M. Pederson, W. X. Li and B. Hammer, PCCP 8, 1566 (2006)
Surface Oxide Bulk PtO2
Barrier: ~ 2 eV
Barrier: 0.2 eV Barrier: 0.3 eV
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Oxidation of Ag(111) and ethylene epoxidationOxidation of Pt(332) and CO OxidationOxidation of Pt(110) and CO OxidationOxidation of Rh(110) and H2 Reduction
Sc Ti V Cr Mn Fe Co Ni Cu Zn
Y Zr Nb Mo Tc Ru Rh Pd Ag Cd
La Hf Ta W Re Os Ir Pt Au Hg
high local oxygen coveragestrained
nanostructured
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- strained nanostructure
increased Rh-Rh dist. (11%)
2 Rh atoms out of 10 ejected
Characteristics of the (10×2) structure
(2×1)p2mg
(10×2)
- reconstructed areas+
unreconstructed areascovered by (2×1)p2mg-O
53×53 Å2
Africh, Esch, Li, Corso, Hammer, Rosei, and Comelli, Phys. Rev. Lett. 93, 126104 (2004)
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H2 Reduction: Two-Step Reaction
40x30nm2
Acquisition time: 35 s per image
Africh, Esch, Li, Corso, Hammer, Rosei, and Comelli, Phys. Rev. Lett. 93, 126104 (2004)
Room temperature, partial pressure of H2: 10-8 mbar
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1st-step reaction
1st oxygen removal:- reaction front- zig-zag oxygen left- strain removal
Initial surface: (10x2)
150 x 150 Å2
Distance between the
segments increased:
no more strain!
40 x 50 Å2
Zig-zaged appearance due to oxygen in threefold sites
(2×2)p2mgsegmented
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2nd-step reaction
1st oxygen removal:- reaction front- zig-zag oxygen left- strain removal
Final surface: clean, segmented (1x2)
150 x 150 Å2
2nd oxygen removal:- homogeneous nucleation
Brighter areas where zig-zag oxygen reacted off
(2×2)p2mgsegmented
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1st Step reactionHH2 2 dissociation barrier:dissociation barrier:•• island edge: 0.23 eVisland edge: 0.23 eV•• middle part and RV between middle part and RV between segments: larger than 0.67 eV segments: larger than 0.67 eV
OH formation barrier:OH formation barrier:•• island edge: 0.78 eVisland edge: 0.78 eV•• middle part and RV between middle part and RV between segments: 0.92 eV and 1.16 eV segments: 0.92 eV and 1.16 eV
H2 Dissociation barrier on Rh(110)-(1x2) less than 0.1 eV
Africh, Esch, Li, Corso, Hammer, Rosei, and Comelli, Phys. Rev. Lett. 93, 126104 (2004)
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Wavefront Formation
AA
DD
BB
CC
OO’’s Stability:s Stability:••Site A: 1.85 eVSite A: 1.85 eV••Site B: 1.85 eVSite B: 1.85 eV••Site C: 1.36 eVSite C: 1.36 eV••Site D: 1.98 eVSite D: 1.98 eV
zigzig--zag structure preferredzag structure preferred
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Wavefront Formation
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2nd Step Reaction
2nd oxygen removal:- homogeneous nucleation
H2 dissociates barrier: 0.12 eVH2 dissociates barrier: 0.12 eVH atom can only adsorb between the ridgeH atom can only adsorb between the ridge
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Conclusion• It is mandatory to study the catalytic reaction under realistic
condition by various experimental and theoretical apparatus, which have to be applied simultaneously, to unravel the active sites, structures and reaction mechanism.
• To do so, in situ facilities and theoretical simulation including temperature and pressure as well as statistics mechanics (KMC) have to be applied or developed.
• Defects (step) and surface orientations has significant impact to the formation of (surface) oxide, reaction mechanism, materials dependent, and therefore has to be studied case by case, in term of bridging so-called pressure and materials gap.
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Xinghai Square, Dalian
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Acknowledgments
Funding: Danish Research CouncilChinese Academy of Sciences Natural Science Foundation of ChinaMax Planck Society
(MPG-CAS Partner Group)
FHI, BerlinCathy Stampfl,Karstern ReuterMatthias Scheffler
University of Lund, SwedenJ. AndersenE. Lundgren O/Pt Core level shift
University of Aarhus, Denmark Bjork HammerEbbe VestergaardStig HelvegF. BesenbacherO/Pt/DFT/STM
Dalian Institute of Chemical PhysicsMingmei Yang / Zhenhua ZengHaiyan Su / Tao Jiang / Xiufang Ma Dr. Xin Liu / Keju Sun