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Sub-Monolayer Sn/Cu(100)

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ZnTPP3 ZnTPP1 on TiO2 No apparent band shift in XPS ZnTPP1 on TiO2 3.4 eV 0.2 eV LUMO LUMO + 1 ZnTPP1 TiO2 HOMO 2.6 eV 2.1 eV ZnTPP1 on TiO2 Normalization ... – PowerPoint PPT presentation

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Title: Sub-Monolayer Sn/Cu(100)


1
Zinc Tetra Phenyl Porphyrin Chromophores
February 2009
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
Zn-TetraPhenylPorphyrin
  • Zn-TPP exhibit a long-lived (gt1ns) p excited
    state
  • Appropriate HOMO/LUMO levels position in energy.
  • Functional groups have not much influence on the
    TPP electronic structure.

ZnTPP Zinc TetraPhenylPorphyrin
4
Energy levels alignment
5
Experimental setup
Occupied and unoccupied states in the same UHV
system
6
First results
7
Zn-based dyes
ZnTPP2
ZnTPP1
These dye are believed to adsorb perpendicular to
the substrate and might form clusters of parallel
molecules.
8
Zn-based dyes
ZnTPP3
This dye is believed to adsorb flat on the
substrate.
9
ZnTPP1 on TiO2
10
ZnTPP1 on TiO2
No apparent band shift in XPS
11
ZnTPP1 on TiO2
12
  • Compared to a multilayer DOS, same main
    characteristics with slightly different weight.
  • Broadening of the principal features could be
    related to
  • the lack of resolution
  • molecular interaction
  • substrate influence
  • photon energy

40.8 eV
Electronic structure and molecular orientation of
a Zn-tetra-phenyl porphyrin multilayer on Si(111)
C. Castellarin Cudia et al.
90 eV
13
Comparison with other methods
14
Reproducibility of results
  • Variability between samples even when using the
    same dying procedure.
  • Broadening of the principal features could be
    related to order on the surface.

15
ZnTPP1 on ZnO(11-20)
Normalization to the substrate chosen to obtain
similar molecular DOS after subtraction of the
substrate contribution to the total DOS.
TiO2(110)
ZnO(11-20)
16
Comparison Zn-TPP derivatives
UPS He II
ZnTPP1
ZnTPP2
HOMO
ZnTPP3
  • Roughly the same features are found for the three
    dyes. In particular, HOMO at the same position in
    the three cases.
  • Effect of adsorption mode difficult to interpret
    in terms of electronic structure. No obvious
    dependence.

17
Comparison Zn-TPP derivatives
ZnTPP1
IPS
ZnTPP2
ZnTPP3
  • Very different results from one dye to another.
    Need to be checked one more time.
  • Effect of adsorption mode difficult to interpret
    in terms of electronic structure. No obvious
    dependence.

18
Next steps
  • Quantitative analysis of all the XPS data for
    coverage determination.
  • Better understanding of the free ZnTPP electronic
    structure to anticipate the modifications of the
    DOS as a function of the adsorption geometry.
  • Ab-initio electronic structure calculation
    (GAMESS)
  • Literature?...
  • Using the low cross section of Zn sp states in
    ZnO CB would allow a better characterization of
    the unoccupied molecular states.

ZnTPP1
19
Next steps
  • STM imaging of individual molecules on a pivalic
    acid passivated surface.
  • Spectroscopic measurements (XPS-UPS-IPS) with
    prior pivalic acid passivation of the surface.

20
DOS from calculated MO
Ph
Zn 3d
Ph
Ph
R
R
HOMO
LUMO
21
ZnP molecular orbitals
HOMO1
LUMO
HOMO
LUMO1
Zn 3d
dyz
dzx
dz2
22
ZnTPP molecular orbitals
HOMO1
LUMO
LUMO1
HOMO
LUMO3
23
ZnTPP vs ZnP molecular orbitals
ZnTPP
ZnP
24
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25
Pivalic acid covered surface
6 Ã…
3 nm x 2 nm
15 nm x 15 nm
26
ZnTPP3 covered surface
15 Ã…
50 nm x 50 nm
30 nm x 30 nm
27
Porphyrin as a model dye
eg
LUMOs
Energy states
HOMOs
Soret (B) band
S2
Q bands
S1
a2u
a1u
S0
28
Zn Tetra Phenyl Porphyrin derivatives
ZnTPP1
29
ZnTPP vs ZnP molecular orbitals
30
Approaches for band alignment tuning 1/3
31
Approaches for band alignment tuning 2/3
32
Approaches for band alignment tuning 2/3
33
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