Upload
others
View
3
Download
0
Embed Size (px)
Citation preview
1
1
Surface Studies of Semiconducting MetalOxides
Ulrike DieboldDepartment of Physics, Tulane University, New Orleans, U.S.A.
or:
Oxides, STM, and DFT:A Happy Marriage
2
Surfaces of Metal Oxides:
• Most metals are oxidized in the ambient.• Metal oxides exhibit an extremely wide
variation in their chemical and physicalproperties (e.g., superconductors to best insulators)
• Metal oxides are important for manyapplications. (And surfaces are critical in most ofthem.)
• Surfaces of metal oxides are challenging(different phases, prepration /chemical potentialdependent surfaces…)
• Defects are important!– Local probes (STM) + DFT + spectroscopies
2
3
TiO2 (mostly)
(some SnO2)
4
Titanium - Oxygen Phase Diagram
4
7
Stability of Polar Surfaces Electrostatic Considerations:
(P.W. Tasker, J. Phys. C 12 (1979) 4977 More recent and improved: Noguera, Jackowski)
type 1: One-layer repeat unit
! = 0,
dipole moment µ =0
+ - + -
+ - + -
+ - + -
+ - + -
+ - + -
+ - + -
+ - + -
type 2: 3-layer symmetrical
repeat unit
! = 0,
dipole moment µ =0
-
2+
--
2+
-
-
+
-+
-
+
type 3: two
-layer repeat unit
! ! 0,
dipole moment µ ! 0
very stable. stable.
generally very unstable.
Rocksalt (100):CaF2 (111):
a
c
a = 3.25 Å
c
ZnO (0001):
8
[110]
[110]
[001]
TiO2 Rutile (110)
OTi
5
9
Interest in TiO2
U. Diebold. “The Surface Science of Titanium Dioxide”, Surf. Sci. Rep. 48 (2003) 53 - 229
10U. Diebold. “The Surface Science of Titanium Dioxide”, Surf. Sci. Rep. 48 (2003) 53 - 229
0
20
40
60
80
100
120
1975 1980 1985 1990 1995 2000 2005 2010
Publications on TiO2(110)
Num
ber o
f P
ublications
Year
/year
0
50
100
150
200
250
300
2002 2003 2004 2005 2006 2007 2008
Citations to U. Diebold, Surf. Sci. Rep. 2003
Num
ber
of
Citations
Year
/year
Interest in TiO2
6
11
TiO2
Optical Properties(pigment in paints,cosmetics, opticalcoatings,photonic material)
Biocompatibility(dental and bone implants)
A
BChemical properties(heterogeneouscatalysis, oxidationreactions at lowtemperatures)
Photo-active material(self-cleaning coatings, solarcells,production of H2)
magnetic properties
?
Electronic properties(gas sensing )
1 µm
12
Message # 1
• Metal oxides (particularly TiO2) areworth your while
• For binary oxides: cut one Me -> Oper O -> me bond.
7
13
Exception to Message # 1(bond cutting):
• SnO2.
14
1mm
(110)
Prof. R. Helbig (Erlangen)
SnO2 has the rutilestructure
(101) or (011)
(110)
M. Batzill, K. Katsiev, and U. D. , Surf. Sci. , 529/3 (2003) 295M. Batzill, K. Katsiev, J.M. Burst, U. D., A. M. Chaka, and B. Delley,Phys. Rev. B, 72 (2005) 165414
8
15
Two surface terminations for SnO2(101):
O2-
Sn4+
The surface maintains a Sn4+O22-
stoichiometry
O-terminated surface:
Sn (5s25p2) has two stable oxidation states (+2,+4)
SnO2 and SnO are stable
Sn-terminated surface:
O2- Sn2+
Sn2+O2- stoichiometry at thesurface.
16
Oxygen terminated surface:10 mbar O2 at RT
Tin terminated surface:sputtered and annealed in UHV
60 eV106 eV
reversible
He+ ISSHe+ ISS
M. Batzill, A.M. Chaka, U. Diebold, Europhysics Lett. 65 (1) (2004) 61
9
17
…much of the surface chemistry of metal oxide isdefect-driven…
V. Henrich, P.A. Cox, “The Surface Science of Metal Oxides” CambridgeUniversity Press 1994
Surface Science:
Oxygen VacanciesHydroxyls
Impurities
Step edges
Shear plances
…
‘The ‘Real World’:
Step Edges
ImpuritiesHydroxyls Oxygen Vacancies
….
18
[110]
[110]
[001]
Rutile (110)
Oxygen Vacancy (Point Defect)
OTi
Relaxations? -- Charlton et al, PRL 78 (1997) 495Ramamoorthy und Vanderbilt, Phys. Rev. B 49 (1994)16721Harrison et al. Faraday Discuss. 114 (1999) 305-312- LEED study (Thornton et al.) -> DFT is correct
10
19
Rutile TiO2(110)point defect
Ti(5)O(3)
O(2)
Oxygen Vacancies: Changed Electronic StructureBand Gap StateClearly Ti 3d- derived
UV Photoelectron Spectroscopy of the Valence Band Region
e-
h"
Experimental:
0
0.2
0.4
0.6
0.8
1
0246810
count s
/s nor m
alize
d to flux
Binding energy (eV)
Clean Surface,annealed in UHV
Defect State
h" = 45 eV
20
Scanning Tunneling Microscopy
• Annealing in ultrahigh vacuum createsmissing oxygen atoms
• Point defects very reactive
• 5 - 10% Ovac, then reconstructions
U.D., J.F. Anderson, K.-O. Ng, D. Vanderbilt, PRL 77 (1996) 1322
• The image contrast in empty-states
STM is reversed to the
morphological topography
11
21
Adsorption of Water:
Experiment:Molecular adsorption,dissociation only at defektsBrinkley et al, Surf. Sci. 395 (1998) 292;Henderson, Langmuir 12 (1996) 5093;Hugenschmid et al. Surf. Sci. 302 (1994)329
600500400300200100
Temperature (K)
1
.5
0
2.5 ML H2O/TiO2(110)TPD, m/e = 18
490
265
163
332
175
m/e
=1
8 Q
MS
sig
na
l (x
10
6c/s
)
Multilayers
2nd layer H2O (H-bonded to Obridging)
1st layer water(molecular at
terraces)
dissociatedat O vacanciesAdsorpti
on at
stepedges?
Henderson, Surf. Sci. 400 (1998) 203
Theory:mixed molecular/dissociativeadsorptionLindan, Harrison, Gillan, Kresse, Noguera,Vogtenhuber, Vittadini, Pacchioni, Casarin,Fahmi & Minot, Ferris, Bredow, Jug,Stefanovich & Truong, Langel, Nørskov,...
22
Rutile TiO2(110) point defect
Ti(5) O(3)
O(2)
Bikonda et al. Nature Materials 5 (2006) 176
Oxygen vacancies on TiO2:Water has a unity stickingcoefficient [1] anddissociates at O vacancies=> easily hydroxylated
[1] T. Engel et al, Surf. Sci.395 (1998) 292
12
23
Photoemission of Water Adsorption on TiO2(011)-2x1 at 110 K:
h" = 26 eVDifference Spectra
h" = 47 eV
2 04
Band gap state increases andshifts with initial wateradsorption
Di Valentin et al, JACS127 (2005) 9895; Beck et al, Surf. Sci. Lett. 591 (2005) L267
24
Electronic structure of O vacancies and OH groups
Hybrid B3LYP functionals describelocalized gap state (C. Di Valentin, A. Selloni,
G. Pacchioni, PRL 2006)
Di Valentin et.al. PRL 2006 submitted
Oxygen vacancy
OH group
Ganduglia-Pirovano, et al.Surf. Sci Rep. 2007
13
25
Message # 2Defects (O vacancies) areimportant, yet challenging
• Theorists: Mistrust theexperimentalists
• Experimentalists: Mistrust thetheorists.
26
Exception to Message # 2(reduced surfaces are reactive)
• SnO2.
14
27
8 6 4 2 00
20
40
60
80
2.6 eV
h! = 34 eV
Counts
[a.u
.]
Binding energy [eV]
573 K 673 K 773 K 873 K 973 K
8 6 4 2 00
20
40
60
80
2.6 eV
h! = 34 eV
Counts
[a.u
.]
Binding energy [eV]
573 K 673 K 773 K 873 K 973 K
8 6 4 2 00
20
40
60
80
2.6 eV
h! = 34 eV
Counts
[a.u
.]
Binding energy [eV]
573 K 673 K 773 K 873 K 973 K
8 6 4 2 00
20
40
60
80
2.6 eV
h! = 34 eV
Counts
[a.u
.]
Binding energy [eV]
573 K 673 K 773 K 873 K 973 K
Temperature
Ultraviolet Photoemission Spectroscopy
M. Batzill, et al. Phys. Rev. B 72 (2005) 165414
Sn-5s
derived
surface
state
8 6 4 2 00
20
40
60
80
2.6 eV
h! = 34 eV
Counts
[a.u
.]
Binding energy [eV]
573 K 673 K 773 K 873 K 973 K
Sn4+
Sn2+
SnO2
28
8 6 4 2 00
20
40
60
80
2.6 eV
h! = 34 eV
Counts
[a.u
.]
Binding energy [eV]
573 K 673 K 773 K 873 K 973 K
Sn-5s derived
surface state
Sn2+
Reduced SnO2 surface:
Is quite inert!
- Water physisorbsM. Batzill, et al., Surf. Sci. 600 (2006) L29; J.Phys. C., 18 (2006) L129-L134
-Benzene interacts veryweaklyM. Batzill et al., Applied Physics Letters, 85(2004) 5766
15
29Eads = -1.518 eV
Undercoordinated Oxygen
may act as Brønsted-base
sites=> dissociation of water
Water adsorption on oxidized and reduced SnO2(101) surfaces:
Fully coordinated Oxygen
Sn2+ cations with
chemically inert Sn-
5s lone pair.
DFT calculations by W. Bergermayer and I. Tanaka,
University of Kyoto, Japan
Eads = -0.989 eV Eads = -0.366 eV
M. Batzill, et al., Surf. Sci. 600 (2006) L29; J. Phys. C., 18 (2006) L129-L134
30
TiO2-Color Scheme
M. Li, et al., Journal of Physical Chemistry B 104 (20) (2000)4944
samples annealed in afurnace(Ar with 20ppm O2 ~4x10-3 Torr)
16
31
[110]
[110]
[001]
Defects in TiO2-x Rutile (110)
Tiinterstitial
Ovac
32
Reduced Crystals - (1x2) Reconstruction
(1x1) with point defects
(1x2)strands
Added Ti2O3 rows - model for (1x2)reconstructionH. Onishi and Y. Iwasawa, Surf. Sci. 313,L783-L789 (1994).
18
35
Message # 3
• Theorists: Think before you useordered O vacancies to modelreconstructions.
• Experimentalists: Don’t trust modelswith ordered vacancies.
36
Ti18O2
Tiinterstitial
18O2
Re-oxidation of reduced TiO2 crystals:
19
37Pan, Maschhoff, Diebold, Madey, JVSTA 10 (1992) 2470 - 2476
38
20
39
Reoxidation of reduced TiO2(110) singlecrystals: cycles (1x1) -> (1x2) structure
R.A. Bennett et al, Phys. Rev. Lett. 82 (1999) 3831
40
Kinetics of re-oxidation:LEEM (see Gary Kellog et al.)
Consequence:Adsorption of reactive species atelevated temperatures can reactwith subsurface defects
22
43
TiO2:
CFM Continental Fan
• removal of organic pollutants, purifying of water or air
titaniumart.com
• self-cleaning/desinfecting coatings (bacteria, viruses, cancer cells)
Sustainable Technologies International
• solar cells
•photocatalytic splitting ofwater, production of hydrogen
TiO2 -based Photocatalysis: Applications and Promise
44
Ohno et al. New J. Chem. 26 (2002) 1167
TiO2-based Photocatalyst
23
45
How about anatase?
46
TiO2 Anatase
(011)
(011)(101)
(101)
(001)
Calculated Wulff ShapeM. Lazzeri, A. Vittadini and A. Selloni, Phys. Rev. B,65 (2002) 119901/1, ibid. Phys. Rev. B, 63 (2001)155409/1
Natural Mineral Sample fromHangarsvidda, Norway
U. Diebold et al. Catalysis Today (2003)
24
47
STM of TiO2 Anatase (101)
no evidence for point defects!
W. Hebenstreit, N. Ruzycki, G.S. Herman, and U.D., PRB Rapid Comm. 64 (24) (2000) R16334
48
H2O/Rutile(110):
600500400300200100
Temperature (K)
1
.5
0
2.5 ML H2O/TiO2(110)TPD, m/e = 18
490
265
163
332
175
m/e
=1
8 Q
MS
sig
na
l (x
10
6c/s
)
Multilayers
2nd layer H2O (H-bonded to Obridging)
1st layer water(molecular at
terraces)
dissociatedat O
vacancies
Adsorpt
ion atstep
edges?
Henderson, Surf. Sci. 400 (1998) 203
m/e
= 2
0 I
nte
nsity (
arb
. u
nits)
500400300200100
Temperature (K)
D2O Exposure
(molecules/cm2, x 10
14)
0 (bkgd)
1.73.45.16.88.5
10.211.913.615.3
250 K
190 K
160 K
H2O/Anatase(101):
G.S. Herman, et al. J. Phys. Chem.B 107 (2003) 2788;A. Selloni, et al, Surf Sci 402-404 (1998), 219
ca. 1 H2O/Ti(5)
25
49
STM of H2O/TiO2 Anatase:
coming soon!
50
Lessons - Surfaces of Metal Oxides
(mainly TiO2):
Defects are important:
Oxygen vacancies (challenging, theoretically andexperimentally)
Hydroxyls
Bulk - surface interplay
Step edges at oxides - interesting area of future research
TiO2 and other oxides: non-polarity of surfaces is good
guidance for predicting surface structure. Consider chemical
potential (gas phase)