2,967 research outputs found
Coverage Dependence of the Level Alignment for Methanol on TiO(110)
Electronic level alignment at the interface between an adsorbed molecular
layer and a semiconducting substrate determines the activity and efficiency of
many photocatalytic materials. We perform calculations to determine
the coverage dependence of the level alignment for a prototypical
photocatalytic interface: 1/2 and 1 monolayer (ML) intact and dissociated
CHOH on rutile TiO(110). We find changes in the wavefunction's spatial
distribution, and a consequent renormalization of the quasiparticle energy
levels, as a function of CHOH coverage and dissociation. Our results
suggest that the occupied molecular levels responsible for hole trapping are
not those observed in the ultraviolet photoemission spectroscopy (UPS)
spectrum. Rather, they are those of isolated CHO on the surface. We find
the unoccupied molecular levels have either 2D character with weight above the
surface at 1 ML coverage, or significant hybridization with the surface at 1/2
ML coverage. These results suggest the resonance observed in the two photon
phooemission (2PP) spectrum arises from excitations to unoccupied "Wet
electron" levels with 2D character.Comment: 8 pages, 5 figures, 1 tabl
Using surface plasmonics to turn on fullerene's dark excitons
Using our recently proposed Bethe-Salpeter formulation, we explore
the optical absorption spectra of fullerene (C) near coinage metal
surfaces (Cu, Ag, and Au). We pay special attention to how the surface plasmon
influences the optical activity of fullerene. We find the lower
energy fullerene excitons at 3.77 and 4.8 eV only weakly interact with the
surface plasmon. However, we find the surface plasmon strongly interacts with
the most intense fullerene exciton, i.e.\ the dipolar mode at
6.5 eV, and the quadrupolar mode at
6.8 eV. When fullerene is close to a copper surface
( 5.3 \AA) the dipolar mode and "localized" surface
plasmons in the molecule/surface interface hybridize to form two coupled modes
which both absorb light. As a result, the molecule gains an additional
optically active mode. Moreover, in resonance, when
, the strong interaction with the surface plasmon
destroys the quadrupolar character and it becomes an optically
active mode. In this case the molecule gains two additional very intense
optically active modes. Further, we find this resonance condition, , is satisfied by silver and gold metal surfaces.Comment: 10 pages, 8 figure
Using Level Alignment to Identify Catechol's Structure on TiO(110)
We perform state-of-the-art calculations for a prototypical dye sensitized
solar cell: catechol on rutile TiO(110). Catechol is often used as an
anchoring group for larger more complex organic and inorganic dyes on TiO
and forms a type II heterojunctions on TiO(110). In particular, we compare
quasiparticle (QP) with hybrid exchange correlation functional (HSE)
density functional theory (DFT) calculations for the catechol-rutile
TiO(110) interface. In so doing, we provide a theoretical interpretation of
ultraviolet photoemission spectroscopy (UPS) and inverse photoemission
spectroscopy (IPES) experiments for this prototypical system. Specifically, we
demonstrate that the position, presence, and intensity of peaks associated with
catechol's HOMO, intermolecular OHO bonds, and interfacial hydrogen bonds to
the surface bridging O atoms (OHC and OHO) may be used to
fingerprint deprotonation of catechol's OH anchoring groups. Furthermore, our
results suggest deprotonation of these groups, while being nearly isoenergetic
at high coverages, may significantly increase the photovoltaic efficiency of
catecholTiO(110) interfaces.Comment: 7 pages, 4 figures, corrected table
European Court of Human Rights: May 2012-April 2013
Analysis of jurisprudential and institutional developments
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