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Sub-Monolayer Sn/Cu(100)

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Energy level alignment of N3 on TiO2(110) and ZnO(11-20) N3 on TiO2 nanoparticles and ZnO nanorods INA vs N3: ... – PowerPoint PPT presentation

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Title: Sub-Monolayer Sn/Cu(100)


1
Electronic Energy Levels Alignment of Dye
Sensitized Oxide Surfaces
Sylvie Rangan Rutgers University Department of
Physics and Astronomy 136 Frelinghuysen Road,
Piscataway, NJ 08854
2
Introduction
A Dye Sensitized Solar Cells (DSSCs) a potential
low cost alternative to Si solar cells.
  • -Sunlight enters the structure,
  • excites electron-hole pairs
  • in dye.
  • -Electron is transferred into
  • TiO2 conduction band, and
  • hole is filled by I- ions
  • (3I- ? 2e- I3-).
  • -Electron travels through circuit,
  • reduces I3- (2e- I3- ? 3I-)

3
Energetics N3 molecule on TiO2
4
New experimental approach of the subject
A few examples to show you it works!
5
Experimental setup
Occupied and unoccupied states in the same UHV
system
6
Experimental setup
Scanning Tunnel Microscope
I
VT-SPM OMICRON
7
Outline
8
Outline
Band alignment tuning strategies
9
TiO2 (110) monocrystal
10
TiO2 (110)
11
N3 on TiO2 (110)
12
Energy diagram
LUMO 1
LUMO
0.5 eV
3.2 eV
Ti3d
HOMO
0.9 eV
LUMO
HOMO
TiO2(110)
N3 TiO2(110)
N3
TiO2
13
Influence of intermediate steps
HOMO and LUMO due to N3
14
Anatase TiO2 nanoparticles
Ti3d
TiO2 nano
N3 TiO2 nano
Dunbar P. Birnie III group, Rutgers University
  • Same HOMO-LUMO gap
  • Anatase gap 0.2 eV larger
  • than rutile gap

100 Ã…
15
Comparison with DSSC perfomances
Incident Photon to Current conversion Efficiency
N3nanocrystals TiO2
From Photoelectrochemical cells, Michael Grätzel,
Nature, nov 2001, 338
16
ZnO substrates
Monoatomic step edge 2 Ã…
100 nm x 100 nm
Length (nm)
ZnO (11-20) epitaxial film
  • ZnO nanorods
  • Grown by Metalorganic
  • chemical vapor deposition
  • Length 1.8 µm
  • Diameter 100 nm

Yicheng Lu group, Rutgers University
17
N3 on ZnO(11-20)
18
N3 on ZnO - nanorod
LUMO 1
LUMO
2.7 eV
2.0 eV
(2.1 eV)
0.4 eV
(0.4 eV)
4.5 eV
Zn3d
O2p
(4.6 eV)
3.4 eV
(3.2 eV)
HOMO
1.3 eV
(1.3 eV)
  • Smaller dye coverage
  • Similar to single crystal ZnO

N3
ZnO
19
Isonicotinic acid N3 linker analogue
20
N3-INA comparison
21
INA on TiO2 model calculations
(1)
(2)
(1) DFT Study of Bare and Dye-Sensitized TiO2
Clusters and Nanocrystals Lundqvist, Nilsing,
Persson, Lunell Intern. Journal of Quantum
Chemistry, Vol 106, 32143234 (2006)
(2) Anchor group influence on moleculemetal
oxide Interfaces Periodic hybrid DFT study of
pyridine bound to TiO2 via carboxylic and
phosphonic acid M. Nilsing , P. Persson, L.
Ojama Chemical Physics Letters 415 (2005) 375380
22
First Conclusion
  • UPS and IPS in the same UHV system
  • The most direct method to characterize the ground
    state electronic structure
  • UV-visible absorption(exciton)/NEXAFS(core hole)
    typically used in the field
  • First measurement of the electronic
    occupied/unoccupied structure of dye molecules on
    surfaces
  • Can help improve theoretical treatment of
    dye/oxides systems.
  • Energy level alignment of N3 on TiO2(110) and
    ZnO(11-20)
  • N3 on TiO2 nanoparticles and ZnO nanorods
  • INA vs N3 linker group good model for LUMO

23
Zn-TetraPhenylPorphyrin
  • Appropriate HOMO/LUMO levels position in energy.
  • Functional groups added to the phenyl groups have
    not much influence on the TPP absorption
    properties.

ZnTPP Zinc TetraPhenylPorphyrin
24
ZnTPP vs ZnP
25
Energy levels alignment
E. Galoppini, Rutgers
26
Approaches for band alignment tuning
27
Approaches for band alignment tuning
28
ZnTPP1 on TiO2
29
Energy level alignment
30
Comparison with other methods 1/2
31
Comparison with other methods 2/2
32
ZnTPP1 electronic structure
33
Tunnel Microscopy Approach
34
ZnTPP3 adsorption
Effect on the electronic structure Adsorption
modes? Aggregation?
35
Another conclusion
ZnTPP derivatives good candidate to study
fundamental properties related to energy level
alignment.
UPS/IPS useful and direct way for measuring
energy level alignment.
Still a lot of work to do!
36
THANKS !!!
37
Absorption properties
Typical UV-visible absorption spectrum
  • S1 and S2 first and second excited states of the
    molecule.
  • Fast internal conversion S2 ? S1
  • B and Q bands both arise from p to p transitions
    and can be explained by considering the four
    frontier orbitals of the porphyrin.

38
Goutermann Four-Orbital Model
Orbitals
LUMOs
HOMOs
Energy states
Soret (B) band
S2
Q bands
S1
  • Transitions between these orbitals gives rise to
    two 1Eu excited states.
  • Orbital mixing splits these two states into a
    high energy state with a high oscillator strength
    and a low energy state with a low oscillator
    strength.

S0
39
Pivalic acid covered surface
6 Ã…
3 nm x 2 nm
15 nm x 15 nm
40
Zn-based dyes
ZnTPP2
ZnTPP1
These dye are believed to adsorb perpendicular to
the substrate and might form clusters of parallel
molecules.
41
Zn-based dyes
ZnTPP3
This dye is believed to adsorb flat on the
substrate.
42
ZnTPP1 on TiO2 and ZnO
Small effect on ZnTPP elecronic structure by
changing the substrate.
43
Approaches for band alignment tuning 3/3
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