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Surfaces of Metal Oxides
Ulrike Diebold
Institute of Applied Physics, TU Wien
Vienna, Austria
DFT Collaborations: Annabella Selloni (Princeton U.), Peter Blaha (TU Wien)
Surfaces of Metal Oxides:
Ulrike Diebold
Institute of Applied Physics, TU Wien
Vienna, Austria
Understanding fundamental
mechanisms and processes at
the atomic scale
&
4
TiO2
U. Diebold,
“The Surface Science of
Titanium Dioxide”,
Surf. Sci. Rep. 48 (2003) 53
[~4000 cites]
Oxide materials we have studied
Fe3O4, In2O3, SrTiO3, Sr3Ru2O7,
SnO2, ZnO, ZrO2
Heterogeneous
Catalysis (support &
active catalyst)
Gas sensing
Photocatalyst
Dye-sensitized
solar cells
Li-ion
batteries
Memristor
Optical Properties
Biocompatibility
&
5
Credits: Forschungszentrum Jülich
Kizuka et al.,
Phys. Rev. B 55, R7398 (1
Main Tool:
Scanning Tunneling Microscopy (STM)*
&
in combination with
Density Functional Theory
6
Credits: Forschungszentrum Jülich
Dulub et al., Science 2007
*Flat, large single crystals. Ultrahigh Vacuum (10-11 mbar), low temperature (6K - 400 K)
Main Tool:
Scanning Tunneling Microscopy (STM)*
&
CREDIT:
VERGRÖSSERUNG
Hinter dieser Scheibeliegt das
HerzdesRastertunelmikrosko
Hier tastet dieNadel
rasterförmigdieProbeab.
Dieresultierende Vergrößerun
50000000-fach.
OKULAR
Kleinesbinokulares
Mikroskop– zur
Positionsüberprüfung
desObjektsundder
tastendenNadel.
OSKOP, FA.C.REICHERT 20 12 RASTERTUNNELMIKROSKOP,TECHN.UNIVERSITÄT WIEN
brauchen zum
n. Dafür spüren
.
ope
he Blutgruppen-Entdecker
einander kombinierte,
Gegenstandoptisch
meter-Abstände auflösen.
spiegel als Lichtlieferant.
Dieser 1Meter hohe Stahkolosswürde heute dasHerz desNobelpreisträgers
Landsteiner höher schlagenlassen:Inder Stahlkammer ertastet eine elektrische
Nadel das Objekt, erkennt Atome anhanddesElektronenstromsundbildet sie als
Schwarz-Weiß-Bildab.Auflösung?500 Milionstel Milimeter. Wichtig:-200° C
Kammertemperatur. Dasfriert die beweglichen Atome einundmacht sie fotogen.
VERGRÖSSERUNG
Luxusanno1890:Drei
optionaleObjektivlinsendirekt
über demzuuntersuchenden
Gegenstand.InKombination
mit der Okular-Linseliefert
diesesMikrsoskopein270-fach
vergrößertesBild.
GEHÄUSE
Robuster Edelstahl.
Schließlichherrscht in
der Kammer auch
Vakuum– um
Verunreinigungenaus
der Luft zuvermeiden.
KÜHLUNG
Über dieseAnschlüsse
wirddieKammer auf
-200°Cabgekühlt -
mittelsflüssigem
Sticksoff.
BELEUCHTUNG
Der Konkavspiegel dient der
Lichbündelungvonuntenauf
denGegenstand.Licht damals?
Tageslicht oder Öllampe.
Sosieht ein Kristall
(Indiumoxid) durchdas
Okular desMikroskops
vonC. Reichert aus.
Sosieht das Kristall auf
einem RTM-Fotoaus:Die
Atome sindhier alsgrau
Kügelchenmühelos
erkennbar.
VERGLEI
Sokleinist d
Lichtmikros
nebendemR
*Flat, large single crystals. Ultrahigh Vacuum (10-11 mbar), low temperature (6K - 400 K)
&
8
1. Adsorption of Oxygen on TiO2
2. Single metal atoms on Fe3O4
&
9
1. Adsorption of Oxygen on TiO2
- O2 does not stick to fully oxidized
surface.
- Needs extra electrons (from oxygen
vacancies, dopants, hydroxyls, etc.)
- Can assume many different
configurations
Oads, (O2
-)ads , (O2
2-)ads , (O2)O
- Role of electric field
&
10
Heterogeneous
Catalysis (support &
active catalyst)
Gas sensing
Biocompatibility
Photocatalyst
M. Haruta,
CatalysisToday 36 (1997)153
Adsorption of Oxygen on TiO2
M. Batzill and UD, Progr. Surf. Sci. 2005
&
TiO2-based Photocatalysis:
The Basic Mechanism
Linsebigler, Lu, Yates, Chem. Rev. 95 (1995) 735
Ohno et al. New J. Chem. 26 (2002) 1167
Photocatalyst: mixture of
TiO2 rutile and anatase
• Rutile and anatase have different photocatalytic activity.
• Under typical photocatalytic conditions, more O2 is adsorbed
on anatase than rutile.
• How does O2 adsorb on TiO2 rutile and anatase?
12
Rutile vs. Anatase: Wulff Shape (DFT Results)
M. Lazzeri, A. Vittadini and A. Selloni, Phys. Rev. B, 65
(2002) 119901/1, ibid. Phys. Rev. B, 63 (2001) 155409/1
Ramamoorthy and Vanderbilt
Phys. Rev. B 49, 16721 (1994)
• Rutile and anatase have different photocatalytic activity.
• Under typical photocatalytic conditions, more O2 is adsorbed
on anatase than rutile.
• How does O2 adsorb on TiO2 rutile and anatase?
13
TiO2- Color Scheme
(Rutile Samples)
M. Li, et al., Journal of Physical Chemistry B 104 (20) (2000)4944
Samples heated in
furnace to different
temperatures
(Ar with 20 ppm O2
~4x10-3 Torr)
Diebold, Li, and Schmid
Annual Rev. Phys. Chem 2010
Ti5c O2c
VO
OH
[110]
[001]
O3c
TiO2 Rutile (110): Model & Scanning Tunneling Microscopy
S.-C. Li, et al., JACS 130, 9080 (2008)
14
Empty-states STM image
Vsample=+0.8 V, const. height, T=78 K
15
TiO2-x +
… see groups of Henderson, Iwasawa, Bowker, Yates, Thornton, Besenbacher,
Wendt, Dohnalek, Kummel, Selloni, Hammer, …
O2O2
Wendt et al. Science 2007
16
Ph. Scheiber et al., Phys. Rev. Lett., 105 (2010) 216101
Vsample=+1.8 V,
I = 0.03 nA,
Tsample = 17 K
17
Natural Mineral Sample from
Hangarsvidda, Norway
U.D. et al., Catalysis Today, 85 (2003) 93-100.
Vendor of cut and polished
anatase(101) samples
(minerals):
http://www.surfacenet.de
TiO2 anatase (Wulff shape)
18
(c)
STM of cleaved* Anatase (101)
Anisotropic step edges
(Gong et al, Nature Mater. 2006)
[10
]1
[010]
300 Å x 300 Å, Vs=+1.3V, It=1.9 nA
*Dulub and Diebold, J. Phys. Cond. Mat. 2010
Adsorption of water
(He et al, Nature Mater. 2009)
No surface oxygen vacancies
(He et al, PRL 2009)
19
DFT Calculations*:
He et al. PRL 2009
Eact for diffusion
(Nudged elastic band, 19 configurations)
V1 -> V4: 0.74 eV
V4 -> V1: 0.95 eV
‘Stiff surface’
(Vacancies move & stay
below)
*GGA-PBE, 216 atom slab, O=0, Formation energies w/respect to O2 in the gas phase.
5.40 eV
4.15 eV4.73 eV
3.69 eV
3.65 eV
Cheng & Selloni, PRB 2009, J. Chem. Phys. 2009
Diffusion of Ovac’s into TiO2 anatase
(STM images @78K)
After electron irradiation @ 100 K
STM @ 295 K
Ph. Scheiber et al PRL 109 (2012) 136103
0
0.2
0.4
0.6
0.8
1
0 100 200 300 400 500 600
V
O
density(normalized)
Annealing Temperature (K)
STM tip:
Pulling O vacancies back to the surface
+5.2 V, 0.7 nA
+1.0 V, 0.1 nA (78 K)
+1.2 V, 0.1 nA
+0.9 V, 0.12 nA (6 K)
1111
1014
1115
2140
Setvin et al. Science, 341 (2013) 988
STM - tip: induced VO migration
+ VO
-5.2V
-
--
- --
- - --
E
Charges positively because of tip-
induced band bending – reversal of
energetics.
Ballistic electrons – overcoming
kinetic barriers 22D. B. Strukov et al., Nature 453, 80 (2008)
J. O. Lee et al., Nat. Nanotechnology 8, 36 (2013)
Memristor
M. Setvin et al. Science, 341 (2013) 988
Phys. Rev. B. 91 (2015) 195403
Uli Aschauer, Annabella Selloni:
23
*Car-Parrinello, timestep of 5 au, fictitious electron mass 500 au
First-Principles Molecular
Dynamics at T = 200 K* ‘bridging peroxo’:
O2
2- replaces lattice O
Interaction of O2 with (subsurface) O vacancy (VO) in TiO2:
Movie available: Supplement to DOI: 10.1126/science.1239879
Uli Aschauer, Annabella Selloni:
24
‘bridging peroxo’:
O2
2- replaces lattice O:
Interaction of O2 with (subsurface) O vacancy (VO) in TiO2:
Uli Aschauer, Annabella Selloni:
25
‘bridging peroxo’:
O2
2- replaces lattice O:
Interaction of O2 with (subsurface) O vacancy (VO) in TiO2:
Experiment:
VO + O2 → O2
2- bridging
Vo+ O2
2- → O2
2- bridging
Movie available: Supplement to DOI: 10.1126/science.1239879
Summary:
How O2 adsorbs on TiO2
26
Rutile (110): Anatase (101):
O2 + (VO)surface→ Oadatom
(via fragile (O2)bridging intermediate)
O2
2- +(VO)bulk→ O2
2-
bridging
Ph. Scheiber et al ,
Phys. Rev. Lett. 105 (2010) 216101
Phys. Rev. Lett. 109 (2012) 136103
M. Setvin et al.
Science, 341 (2013) 988
Angew. Chem. Int. Ed. 53 (2014) 4714
2nd Topic - Fe3O4(001):
28
M. Haruta, CatalysisToday 36 (1997)153
• How active are the
smallest clusters?
• Single atoms?
• Sintering
• Reaction mechanism
Magnetite Fe3O4 (001)
Bulk: Inverse spinel structure, AB2O4
Tetrahedral Fe(A)3+
Octahedral Fe(B)2.5+
O2- (FCC sublattice)
(001)
(010)
(100)
29
The Reconstructed Fe3O4(001) Surface
In STM we “see” wavy rows of Fe(B) atoms
Vsample = +1 V, Itunnel = 0.35 nA
STM image of the clean surface
Ar+ sputter + anneal 600 °C
1 nm
30
Vapor-deposited
metal adsorbs as
isolated atoms
here
Bulk Termination:
31
R. Bliem, et al. Science 346 (2014) 1212
DFT+U, Ueff = 3.8
The Reconstructed Fe3O4(001) Surface
Maghemite (γ-Fe2O3) defect
32
The Reconstructed Fe3O4(001) Surface
R. Bliem, et al. Science 346 (2014) 1212
Subsurface Cation Vacancy Structure
33DFT+U, Ueff = 3.8
The Reconstructed Fe3O4(001) Surface
LEED-IV: SE > 11 000 eV,
Rpendry = 0.125
R. Bliem, et al. Science 346 (2014) 1212
Adatom Adsorption
• DFT+U: Au adsorbs strongly at one specific site
34
Subsurface Cation Vacancy Structure + Au
Au(I), Eads = 2.03 eV (46 kcal/mol),
DFT+U, Ueff = 3.8
R. Bliem, et al. Science 346 (2014) 1212
Au/Fe3O4(001)
35(30×30 nm2) Vsample = +1 V, Itunnel = 0.38 nA
Isolated Au adatoms
stable at room temperature
nearest neighbour 8.4 Å
no clusters
STM image of 0.12 ML Au
at room temperature (UHV)
Z. Novotny, G. Argentero, Z. Wang, M. Schmid, U. Diebold, G. S. Parkinson
Phys. Rev. Lett. 108, 216103 (2012)
36
Single, Stable Ad-atoms on Fe3O4(001):
Pd/Fe3O4(001)
Pd/Fe3O4(001)
50 x 50 nm2; V=1.2 V ; I=0.3 nA; 0.2 ML Pd in adatoms, 0.2ML in clusters
Adatoms
Clusters
Fuzzy Clusters
(mobile)
G.S.Parkinson et al. Nature Materials 12 (2013) 724
Cluster Coarsening
• The growth of active catalyst material
• A major cause of catalyst deactivation
• Is often thermally driven
• Can also be induced by gas molecules
Michael Bowker, Nature Materials 1, 205 - 206 (2002)
Cluster Coarsening
• The growth of active catalyst material
• A major cause of catalyst deactivation
• Is often thermally driven
• Can also be induced by gas molecules
Michael Bowker, Nature Materials 1, 205 - 206 (2002)
Next: Follow aggregation of
single atoms, step-by-step
STM Movie
(50×50 nm2, +1 V, 0.2 nA)
78 frames, 5.33 hours
0.2 ML Pd/Fe3O4(001)
sample in ultrahigh
vacuum (p < 10-11 mbar)
Room Temperature
Close
Up…
One Pd adatom becomes mobile
Jumps from Pd to Pd across the surface
(6.5×8.5 nm2, +1 V, 0.2 nA)
G.S.Parkinson et al. Nature Materials 12 (2013) 724
PdFeoct
O
2.02 Å
DFT+U (Ueff= 3.8 eV for the Fe-3d states)
Pd atom binds in a Fetet bulk continuation site, 2.2 eV binding energy
Pd is similar to undercoordinated Fetet (2+)
Magnetic moment 0.47 μB
Fetet
Calculations by Rukan Kosak and Peter Blaha, TU Wien
Pd/Fe3O4(001) - Theroy
G.S.Parkinson et al. Nature Materials 12 (2013) 724
CO-Pd/Fe3O4(001) – DFT+U
Pd
C
O
Pd-O bond
broken
2.05 Å
1.86 Å
1.16 Å
CO lifts Pd from surface
Energy gain 1.6 eV
Calculations by Rukan Kosak and Peter Blaha, TU Wien
G.S.Parkinson et al. Nature Materials 12 (2013) 724
• One Pd spontaneously becomes mobile, starts
to diffuse around…
Fe3O4(001)
Pd
Adsorption landscape experienced by Pd atom.
Pd trapped in deep well at “N” sites.
45
• One Pd spontaneously becomes mobile, starts
to diffuse around…
Fe3O4(001)
CO
46
Pd Carbonyl is formed through adsorption of CO
• One Pd spontaneously becomes mobile, starts
to diffuse around…
47
NOTE: This suggests the (Pd carbonyl) – Pd bond is
not strong enough for cluster nucleation.
“skyhook effect”
S. Horch, et al. Nature 398, 134–136 (1999).
CO  Pd/Fe3O4(001)
Pd clusters
270 pm
Dose CO, 100 Langmuir (1.33x10-4 mbar.sec)
OH
CO  Pd/Fe3O4(001)
Dose CO, 100 Langmuir (1.33x10-4 mbar.sec)
270 pm
x x
x
x x
x
x
x
x
x x
x
x
x x
x
x
x
x
No more Pd adatoms.
Large clusters and 270 pm features
CO induces sintering
OH
Pd clusters
Now…since CO causes sintering, we
can tune to an observable rate with
the CO pressure and watch…
WATCH
HERE
Selected Frames…
CO induces mobility in the system
Multiple Pd-CO needed to nucleate cluster
Homogeneous nucleation
Clusters grow through diffusion and coalescence
“Large cluster” contains 19 Pd atoms
(14×14 nm2, +1 V, 0.2 nA)
G.S.Parkinson et al. Nature Materials 12 (2013) 724
Remember the red crosses?
x
x x
x
x
x
x
x x
x
x
x x
x
x
x
270 pm species
(10×10 nm2, +1 V, 0.2 nA)
The Role of Hydroxyls
G.S.Parkinson et al. Nature Materials 12 (2013) 724
Summary
Pd carbonyls are the mobile species
PdCO temporarily trapped at stable Pd adatoms
Homogenous cluster nucleation
Growth through cluster diffusion
and coalescence
OH groups stabilize Pd adatoms
against CO induced mobility
G.S.Parkinson et al. Nature Materials 12 (2013) 724
58
Single, Stable Ad-atoms on Fe3O4(001):
59
Single, Stable Ad-atoms on Fe3O4(001):
M. Haruta, CatalysisToday 36 (1997)153
• How active are the
smallest clusters?
• Single atoms?
• Sintering
• Reaction mechanism
O
O
+ CO
CO
- CO2
Oxygen vacancy 1) CO adsorption on Pt
2) Abstraction of O-lattice
+ 1/2 O2
Reparation of the surface
61
Mars-van Krevelen Mechanism
O
O
+ CO
CO
- CO2
Oxygen vacancy 1) CO adsorption on Pt
2) Abstraction of O-lattice
+ 1/2 O2
PROX reaction*
in excess H2
*Preferential Oxidation of CO in H2 steam
62
Reparation of the surface
Mars-van Krevelen Mechanism
Next: Follow each step individually
For Pt supported on Fe3O4
Pt on Fe3O4(001), after heating to 550 K
1x10-7 mbar CO, 20 min
• Holes in the surface
• Clusters are located
at edges
• Not all clusters have
holes
R. Bliem, et al., Angew. Chem. Intl. Ed 54 (2015) DOI:10.1002/ ange.201507368
Pt on Fe3O4(001), after heating to 550 K
1x10-7 mbar CO, 20 min
O
Fe
O
Fe
O
Fe
O
Fe
O
Fe
O
Fe
O
C
• Holes in the surface
• Clusters are located
at edges
• Not all clusters have
holes
O
Fe
O
Fe
O
Fe
O
Fe
O
Fe
O
Fe
O
C
Fe
O
Fe
O
Fe
O
Fe
O
Fe
O
Fe
CO2
R. Bliem, et al., Angew. Chem. Intl. Ed 54 (2015) DOI:10.1002/ ange.201507368
Pt on Fe3O4(001), after heating to 550 K
1x10-7 mbar O2, 10 min
• Hillocks around each cluster
Growth of Fe3O4:
• O2 adsorption, dissociation,
and spillover
• Reaction with excess Fe
from the bulk
R. Bliem, et al., Angew. Chem. Intl. Ed 54 (2015) DOI:10.1002/ ange.201507368
Pt on Fe3O4(001), after heating to 550 K
1x10-7 mbar O2, 10 min
Fe
O O
-
O
-
O
-
Fe
• Hillocks around each cluster
Growth of Fe3O4:
• O2 adsorption, dissociation,
and spillover
• Reaction with excess Fe
from the bulk
R. Bliem, et al., Angew. Chem. Intl. Ed 54 (2015) DOI:10.1002/ ange.201507368
O
Fe
O
Fe
O
Fe
O
Fe
Fe
O
Fe
CO2
O O
-
O
Fe
O
Fe
O
Fe
Fe
+CO
+O2
etching
re-growth
p CO = 1x10-7 mbar, T = 550 K
R. Bliem, et al., Angew. Chem. Intl. Ed 54 (2015) DOI:10.1002/ ange.201507368
Surfaces of Metal Oxides.

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Surfaces of Metal Oxides.

  • 1. Surfaces of Metal Oxides Ulrike Diebold Institute of Applied Physics, TU Wien Vienna, Austria
  • 2. DFT Collaborations: Annabella Selloni (Princeton U.), Peter Blaha (TU Wien)
  • 3. Surfaces of Metal Oxides: Ulrike Diebold Institute of Applied Physics, TU Wien Vienna, Austria Understanding fundamental mechanisms and processes at the atomic scale
  • 4. & 4 TiO2 U. Diebold, “The Surface Science of Titanium Dioxide”, Surf. Sci. Rep. 48 (2003) 53 [~4000 cites] Oxide materials we have studied Fe3O4, In2O3, SrTiO3, Sr3Ru2O7, SnO2, ZnO, ZrO2 Heterogeneous Catalysis (support & active catalyst) Gas sensing Photocatalyst Dye-sensitized solar cells Li-ion batteries Memristor Optical Properties Biocompatibility
  • 5. & 5 Credits: Forschungszentrum Jülich Kizuka et al., Phys. Rev. B 55, R7398 (1 Main Tool: Scanning Tunneling Microscopy (STM)*
  • 6. & in combination with Density Functional Theory 6 Credits: Forschungszentrum Jülich Dulub et al., Science 2007 *Flat, large single crystals. Ultrahigh Vacuum (10-11 mbar), low temperature (6K - 400 K) Main Tool: Scanning Tunneling Microscopy (STM)*
  • 7. & CREDIT: VERGRÖSSERUNG Hinter dieser Scheibeliegt das HerzdesRastertunelmikrosko Hier tastet dieNadel rasterförmigdieProbeab. Dieresultierende Vergrößerun 50000000-fach. OKULAR Kleinesbinokulares Mikroskop– zur Positionsüberprüfung desObjektsundder tastendenNadel. OSKOP, FA.C.REICHERT 20 12 RASTERTUNNELMIKROSKOP,TECHN.UNIVERSITÄT WIEN brauchen zum n. Dafür spüren . ope he Blutgruppen-Entdecker einander kombinierte, Gegenstandoptisch meter-Abstände auflösen. spiegel als Lichtlieferant. Dieser 1Meter hohe Stahkolosswürde heute dasHerz desNobelpreisträgers Landsteiner höher schlagenlassen:Inder Stahlkammer ertastet eine elektrische Nadel das Objekt, erkennt Atome anhanddesElektronenstromsundbildet sie als Schwarz-Weiß-Bildab.Auflösung?500 Milionstel Milimeter. Wichtig:-200° C Kammertemperatur. Dasfriert die beweglichen Atome einundmacht sie fotogen. VERGRÖSSERUNG Luxusanno1890:Drei optionaleObjektivlinsendirekt über demzuuntersuchenden Gegenstand.InKombination mit der Okular-Linseliefert diesesMikrsoskopein270-fach vergrößertesBild. GEHÄUSE Robuster Edelstahl. Schließlichherrscht in der Kammer auch Vakuum– um Verunreinigungenaus der Luft zuvermeiden. KÜHLUNG Über dieseAnschlüsse wirddieKammer auf -200°Cabgekühlt - mittelsflüssigem Sticksoff. BELEUCHTUNG Der Konkavspiegel dient der Lichbündelungvonuntenauf denGegenstand.Licht damals? Tageslicht oder Öllampe. Sosieht ein Kristall (Indiumoxid) durchdas Okular desMikroskops vonC. Reichert aus. Sosieht das Kristall auf einem RTM-Fotoaus:Die Atome sindhier alsgrau Kügelchenmühelos erkennbar. VERGLEI Sokleinist d Lichtmikros nebendemR *Flat, large single crystals. Ultrahigh Vacuum (10-11 mbar), low temperature (6K - 400 K)
  • 8. & 8 1. Adsorption of Oxygen on TiO2 2. Single metal atoms on Fe3O4
  • 9. & 9 1. Adsorption of Oxygen on TiO2 - O2 does not stick to fully oxidized surface. - Needs extra electrons (from oxygen vacancies, dopants, hydroxyls, etc.) - Can assume many different configurations Oads, (O2 -)ads , (O2 2-)ads , (O2)O - Role of electric field
  • 10. & 10 Heterogeneous Catalysis (support & active catalyst) Gas sensing Biocompatibility Photocatalyst M. Haruta, CatalysisToday 36 (1997)153 Adsorption of Oxygen on TiO2 M. Batzill and UD, Progr. Surf. Sci. 2005
  • 11. & TiO2-based Photocatalysis: The Basic Mechanism Linsebigler, Lu, Yates, Chem. Rev. 95 (1995) 735 Ohno et al. New J. Chem. 26 (2002) 1167 Photocatalyst: mixture of TiO2 rutile and anatase • Rutile and anatase have different photocatalytic activity. • Under typical photocatalytic conditions, more O2 is adsorbed on anatase than rutile. • How does O2 adsorb on TiO2 rutile and anatase?
  • 12. 12 Rutile vs. Anatase: Wulff Shape (DFT Results) M. Lazzeri, A. Vittadini and A. Selloni, Phys. Rev. B, 65 (2002) 119901/1, ibid. Phys. Rev. B, 63 (2001) 155409/1 Ramamoorthy and Vanderbilt Phys. Rev. B 49, 16721 (1994) • Rutile and anatase have different photocatalytic activity. • Under typical photocatalytic conditions, more O2 is adsorbed on anatase than rutile. • How does O2 adsorb on TiO2 rutile and anatase?
  • 13. 13 TiO2- Color Scheme (Rutile Samples) M. Li, et al., Journal of Physical Chemistry B 104 (20) (2000)4944 Samples heated in furnace to different temperatures (Ar with 20 ppm O2 ~4x10-3 Torr)
  • 14. Diebold, Li, and Schmid Annual Rev. Phys. Chem 2010 Ti5c O2c VO OH [110] [001] O3c TiO2 Rutile (110): Model & Scanning Tunneling Microscopy S.-C. Li, et al., JACS 130, 9080 (2008) 14 Empty-states STM image Vsample=+0.8 V, const. height, T=78 K
  • 15. 15 TiO2-x + … see groups of Henderson, Iwasawa, Bowker, Yates, Thornton, Besenbacher, Wendt, Dohnalek, Kummel, Selloni, Hammer, … O2O2 Wendt et al. Science 2007
  • 16. 16 Ph. Scheiber et al., Phys. Rev. Lett., 105 (2010) 216101 Vsample=+1.8 V, I = 0.03 nA, Tsample = 17 K
  • 17. 17 Natural Mineral Sample from Hangarsvidda, Norway U.D. et al., Catalysis Today, 85 (2003) 93-100. Vendor of cut and polished anatase(101) samples (minerals): http://www.surfacenet.de TiO2 anatase (Wulff shape)
  • 18. 18 (c) STM of cleaved* Anatase (101) Anisotropic step edges (Gong et al, Nature Mater. 2006) [10 ]1 [010] 300 Å x 300 Å, Vs=+1.3V, It=1.9 nA *Dulub and Diebold, J. Phys. Cond. Mat. 2010 Adsorption of water (He et al, Nature Mater. 2009) No surface oxygen vacancies (He et al, PRL 2009)
  • 19. 19 DFT Calculations*: He et al. PRL 2009 Eact for diffusion (Nudged elastic band, 19 configurations) V1 -> V4: 0.74 eV V4 -> V1: 0.95 eV ‘Stiff surface’ (Vacancies move & stay below) *GGA-PBE, 216 atom slab, O=0, Formation energies w/respect to O2 in the gas phase. 5.40 eV 4.15 eV4.73 eV 3.69 eV 3.65 eV Cheng & Selloni, PRB 2009, J. Chem. Phys. 2009
  • 20. Diffusion of Ovac’s into TiO2 anatase (STM images @78K) After electron irradiation @ 100 K STM @ 295 K Ph. Scheiber et al PRL 109 (2012) 136103 0 0.2 0.4 0.6 0.8 1 0 100 200 300 400 500 600 V O density(normalized) Annealing Temperature (K)
  • 21. STM tip: Pulling O vacancies back to the surface +5.2 V, 0.7 nA +1.0 V, 0.1 nA (78 K) +1.2 V, 0.1 nA +0.9 V, 0.12 nA (6 K) 1111 1014 1115 2140 Setvin et al. Science, 341 (2013) 988
  • 22. STM - tip: induced VO migration + VO -5.2V - -- - -- - - -- E Charges positively because of tip- induced band bending – reversal of energetics. Ballistic electrons – overcoming kinetic barriers 22D. B. Strukov et al., Nature 453, 80 (2008) J. O. Lee et al., Nat. Nanotechnology 8, 36 (2013) Memristor M. Setvin et al. Science, 341 (2013) 988 Phys. Rev. B. 91 (2015) 195403
  • 23. Uli Aschauer, Annabella Selloni: 23 *Car-Parrinello, timestep of 5 au, fictitious electron mass 500 au First-Principles Molecular Dynamics at T = 200 K* ‘bridging peroxo’: O2 2- replaces lattice O Interaction of O2 with (subsurface) O vacancy (VO) in TiO2: Movie available: Supplement to DOI: 10.1126/science.1239879
  • 24. Uli Aschauer, Annabella Selloni: 24 ‘bridging peroxo’: O2 2- replaces lattice O: Interaction of O2 with (subsurface) O vacancy (VO) in TiO2:
  • 25. Uli Aschauer, Annabella Selloni: 25 ‘bridging peroxo’: O2 2- replaces lattice O: Interaction of O2 with (subsurface) O vacancy (VO) in TiO2: Experiment: VO + O2 → O2 2- bridging Vo+ O2 2- → O2 2- bridging Movie available: Supplement to DOI: 10.1126/science.1239879
  • 26. Summary: How O2 adsorbs on TiO2 26 Rutile (110): Anatase (101): O2 + (VO)surface→ Oadatom (via fragile (O2)bridging intermediate) O2 2- +(VO)bulk→ O2 2- bridging Ph. Scheiber et al , Phys. Rev. Lett. 105 (2010) 216101 Phys. Rev. Lett. 109 (2012) 136103 M. Setvin et al. Science, 341 (2013) 988 Angew. Chem. Int. Ed. 53 (2014) 4714
  • 27.
  • 28. 2nd Topic - Fe3O4(001): 28 M. Haruta, CatalysisToday 36 (1997)153 • How active are the smallest clusters? • Single atoms? • Sintering • Reaction mechanism
  • 29. Magnetite Fe3O4 (001) Bulk: Inverse spinel structure, AB2O4 Tetrahedral Fe(A)3+ Octahedral Fe(B)2.5+ O2- (FCC sublattice) (001) (010) (100) 29
  • 30. The Reconstructed Fe3O4(001) Surface In STM we “see” wavy rows of Fe(B) atoms Vsample = +1 V, Itunnel = 0.35 nA STM image of the clean surface Ar+ sputter + anneal 600 °C 1 nm 30 Vapor-deposited metal adsorbs as isolated atoms here
  • 31. Bulk Termination: 31 R. Bliem, et al. Science 346 (2014) 1212 DFT+U, Ueff = 3.8 The Reconstructed Fe3O4(001) Surface
  • 32. Maghemite (γ-Fe2O3) defect 32 The Reconstructed Fe3O4(001) Surface R. Bliem, et al. Science 346 (2014) 1212
  • 33. Subsurface Cation Vacancy Structure 33DFT+U, Ueff = 3.8 The Reconstructed Fe3O4(001) Surface LEED-IV: SE > 11 000 eV, Rpendry = 0.125 R. Bliem, et al. Science 346 (2014) 1212
  • 34. Adatom Adsorption • DFT+U: Au adsorbs strongly at one specific site 34 Subsurface Cation Vacancy Structure + Au Au(I), Eads = 2.03 eV (46 kcal/mol), DFT+U, Ueff = 3.8 R. Bliem, et al. Science 346 (2014) 1212
  • 35. Au/Fe3O4(001) 35(30×30 nm2) Vsample = +1 V, Itunnel = 0.38 nA Isolated Au adatoms stable at room temperature nearest neighbour 8.4 Å no clusters STM image of 0.12 ML Au at room temperature (UHV) Z. Novotny, G. Argentero, Z. Wang, M. Schmid, U. Diebold, G. S. Parkinson Phys. Rev. Lett. 108, 216103 (2012)
  • 36. 36 Single, Stable Ad-atoms on Fe3O4(001):
  • 38. Pd/Fe3O4(001) 50 x 50 nm2; V=1.2 V ; I=0.3 nA; 0.2 ML Pd in adatoms, 0.2ML in clusters Adatoms Clusters Fuzzy Clusters (mobile) G.S.Parkinson et al. Nature Materials 12 (2013) 724
  • 39. Cluster Coarsening • The growth of active catalyst material • A major cause of catalyst deactivation • Is often thermally driven • Can also be induced by gas molecules Michael Bowker, Nature Materials 1, 205 - 206 (2002)
  • 40. Cluster Coarsening • The growth of active catalyst material • A major cause of catalyst deactivation • Is often thermally driven • Can also be induced by gas molecules Michael Bowker, Nature Materials 1, 205 - 206 (2002) Next: Follow aggregation of single atoms, step-by-step
  • 41. STM Movie (50×50 nm2, +1 V, 0.2 nA) 78 frames, 5.33 hours 0.2 ML Pd/Fe3O4(001) sample in ultrahigh vacuum (p < 10-11 mbar) Room Temperature
  • 42. Close Up… One Pd adatom becomes mobile Jumps from Pd to Pd across the surface (6.5×8.5 nm2, +1 V, 0.2 nA) G.S.Parkinson et al. Nature Materials 12 (2013) 724
  • 43. PdFeoct O 2.02 Å DFT+U (Ueff= 3.8 eV for the Fe-3d states) Pd atom binds in a Fetet bulk continuation site, 2.2 eV binding energy Pd is similar to undercoordinated Fetet (2+) Magnetic moment 0.47 μB Fetet Calculations by Rukan Kosak and Peter Blaha, TU Wien Pd/Fe3O4(001) - Theroy G.S.Parkinson et al. Nature Materials 12 (2013) 724
  • 44. CO-Pd/Fe3O4(001) – DFT+U Pd C O Pd-O bond broken 2.05 Å 1.86 Å 1.16 Å CO lifts Pd from surface Energy gain 1.6 eV Calculations by Rukan Kosak and Peter Blaha, TU Wien G.S.Parkinson et al. Nature Materials 12 (2013) 724
  • 45. • One Pd spontaneously becomes mobile, starts to diffuse around… Fe3O4(001) Pd Adsorption landscape experienced by Pd atom. Pd trapped in deep well at “N” sites. 45
  • 46. • One Pd spontaneously becomes mobile, starts to diffuse around… Fe3O4(001) CO 46 Pd Carbonyl is formed through adsorption of CO
  • 47. • One Pd spontaneously becomes mobile, starts to diffuse around… 47 NOTE: This suggests the (Pd carbonyl) – Pd bond is not strong enough for cluster nucleation. “skyhook effect” S. Horch, et al. Nature 398, 134–136 (1999).
  • 48. CO  Pd/Fe3O4(001) Pd clusters 270 pm Dose CO, 100 Langmuir (1.33x10-4 mbar.sec) OH
  • 49. CO  Pd/Fe3O4(001) Dose CO, 100 Langmuir (1.33x10-4 mbar.sec) 270 pm x x x x x x x x x x x x x x x x x x x No more Pd adatoms. Large clusters and 270 pm features CO induces sintering OH Pd clusters
  • 50. Now…since CO causes sintering, we can tune to an observable rate with the CO pressure and watch…
  • 51.
  • 53. Selected Frames… CO induces mobility in the system Multiple Pd-CO needed to nucleate cluster Homogeneous nucleation Clusters grow through diffusion and coalescence “Large cluster” contains 19 Pd atoms (14×14 nm2, +1 V, 0.2 nA) G.S.Parkinson et al. Nature Materials 12 (2013) 724
  • 54. Remember the red crosses? x x x x x x x x x x x x x x x x
  • 55. 270 pm species (10×10 nm2, +1 V, 0.2 nA) The Role of Hydroxyls G.S.Parkinson et al. Nature Materials 12 (2013) 724
  • 56. Summary Pd carbonyls are the mobile species PdCO temporarily trapped at stable Pd adatoms Homogenous cluster nucleation Growth through cluster diffusion and coalescence OH groups stabilize Pd adatoms against CO induced mobility G.S.Parkinson et al. Nature Materials 12 (2013) 724
  • 57.
  • 58. 58 Single, Stable Ad-atoms on Fe3O4(001):
  • 59. 59 Single, Stable Ad-atoms on Fe3O4(001):
  • 60. M. Haruta, CatalysisToday 36 (1997)153 • How active are the smallest clusters? • Single atoms? • Sintering • Reaction mechanism
  • 61. O O + CO CO - CO2 Oxygen vacancy 1) CO adsorption on Pt 2) Abstraction of O-lattice + 1/2 O2 Reparation of the surface 61 Mars-van Krevelen Mechanism
  • 62. O O + CO CO - CO2 Oxygen vacancy 1) CO adsorption on Pt 2) Abstraction of O-lattice + 1/2 O2 PROX reaction* in excess H2 *Preferential Oxidation of CO in H2 steam 62 Reparation of the surface Mars-van Krevelen Mechanism Next: Follow each step individually For Pt supported on Fe3O4
  • 63. Pt on Fe3O4(001), after heating to 550 K 1x10-7 mbar CO, 20 min • Holes in the surface • Clusters are located at edges • Not all clusters have holes R. Bliem, et al., Angew. Chem. Intl. Ed 54 (2015) DOI:10.1002/ ange.201507368
  • 64. Pt on Fe3O4(001), after heating to 550 K 1x10-7 mbar CO, 20 min O Fe O Fe O Fe O Fe O Fe O Fe O C • Holes in the surface • Clusters are located at edges • Not all clusters have holes O Fe O Fe O Fe O Fe O Fe O Fe O C Fe O Fe O Fe O Fe O Fe O Fe CO2 R. Bliem, et al., Angew. Chem. Intl. Ed 54 (2015) DOI:10.1002/ ange.201507368
  • 65. Pt on Fe3O4(001), after heating to 550 K 1x10-7 mbar O2, 10 min • Hillocks around each cluster Growth of Fe3O4: • O2 adsorption, dissociation, and spillover • Reaction with excess Fe from the bulk R. Bliem, et al., Angew. Chem. Intl. Ed 54 (2015) DOI:10.1002/ ange.201507368
  • 66. Pt on Fe3O4(001), after heating to 550 K 1x10-7 mbar O2, 10 min Fe O O - O - O - Fe • Hillocks around each cluster Growth of Fe3O4: • O2 adsorption, dissociation, and spillover • Reaction with excess Fe from the bulk R. Bliem, et al., Angew. Chem. Intl. Ed 54 (2015) DOI:10.1002/ ange.201507368
  • 67. O Fe O Fe O Fe O Fe Fe O Fe CO2 O O - O Fe O Fe O Fe Fe +CO +O2 etching re-growth p CO = 1x10-7 mbar, T = 550 K R. Bliem, et al., Angew. Chem. Intl. Ed 54 (2015) DOI:10.1002/ ange.201507368