7 research outputs found
Magnetocapacitance at the Ni/BiInO<sub>3</sub> Schottky Interface
We report the observation of a magnetocapacitance effect
at the
interface between Ni and epitaxial nonpolar BiInO3 thin
films at room temperature. A detailed surface study using X-ray photoelectron
spectroscopy (XPS) reveals the formation of an intermetallic NiāBi
alloy at the Ni/BiInO3 interface and a shift in the Bi
4f and In 3d core levels to higher binding energies with increasing
Ni thickness. The latter infers band bending in BiInO3,
corresponding to the formation of a p-type Schottky barrier. The currentāvoltage
characteristics of the Ni/BiInO3/(Ba,Sr)RuO3/NdScO3(110) heterostructure show a significant dependence
on the applied magnetic field and voltage cycling, which can be attributed
to voltage-controlled band bending and spin-polarized charge accumulation
in the vicinity of the Ni/BiInO3 interface. The magnetocapacitance
effect can be realized at room temperature without involving multiferroic
materials
Electronic Structure of a Spin Crossover Molecular Adsorbate
We have investigated the occupied and unoccupied electronic
structure
of ultrahigh vacuum (UHV) evaporated molecular thin films of the spin
crossover [FeĀ(H<sub>2</sub>BĀ(pz)<sub>2</sub>)<sub>2</sub>(bipy)] complex
(with H<sub>2</sub>BĀ(pz)<sub>2</sub> = bisĀ(hydrido)ĀbisĀ(1<i>H</i>-pyrazol-1-yl)Āborate and bipy = 2,2ā²-bipyridine) by ultraviolet
photoelectron spectroscopy (UPS), inverse photoemission (IPES), and
X-ray absorption spectroscopy (XAS). A bandgap of 2ā3 eV is
deduced from combined UPS and IPES measurements of the molecular films
on Au substrates. The matching Fe XAS and IPES spectra indicate that
the electronic unoccupied states have a significant Fe weight. The
shift of the unoccupied density of states seen in inverse photoemission
is consistent with the thermally induced spin crossover transition
for [FeĀ(H<sub>2</sub>BĀ(pz)<sub>2</sub>)<sub>2</sub>(bipy)] deposited
on the organic ferroelectric copolymer polyĀ(vinylidene fluoride) with
trifluoroethylene (PVDFāTrFE)
Coverage-Dependent Interactions at the OrganicsāMetal Interface: Quinonoid Zwitterions on Au(111)
The large intrinsic electric dipole
of about 10 D of a <i>p</i>-benzoquinonemonoimine compound
from the class of <i>N</i>-alkyldiaminoresorcinone (or 4,6-bisdialkylaminobenzene-1,3-diones,
i.e., C<sub>6</sub>H<sub>2</sub>(<u>Ā·Ā·Ā·</u> NHR)<sub>2</sub>(<u>Ā·Ā·Ā·</u> O)<sub>2</sub>, where R = H) zwitterions is reduced considerably upon adsorption
on Au(111) substrates. Scanning tunneling microscopy images reveal
parallel alignment of adsorbed molecules within extended islands,
leading to the formation of polarized domains. This is in contrast
to the typical antiparallel alignment found in the bulk. High-resolution
images show that the molecules form rows along the āØ1Ģ
01ā©
directions of the Au(111) surface, but otherwise their arrangement
is only weakly perturbed by the Au(111) (23 Ć ā3) herringbone
surface reconstruction. Density functional theory calculations show
that upon increasing the molecular density the strength of the interaction
between the zwitterions and the Au(111) surface decreases. Thus, the
charge redistribution, which occurs at the interface as a result of
molecular adsorption, and therefore the interfacial dipole is coverage
dependent. The weakening of the interaction at the organicāmetal
interface with increasing coverage is experimentally observed as a
contraction of the intermolecular bond length. Moreover, it is the
strong adsorbateāadsorbate interactions (and not the interactions
between the adsorbate molecules and the surface) which determine the
molecular arrangement within the 2D network the zwitterions form
Altering the Static Dipole on Surfaces through Chemistry: Molecular Films of Zwitterionic Quinonoids
The adsorption of molecular films made of small molecules
with a large intrinsic electrical dipole has been explored. The data
indicate that such dipolar molecules may be used for altering the
interface dipole screening at the metal electrode interface in organic
electronics. More specifically, we have investigated the surface electronic
spectroscopic properties of zwitterionic molecules containing 12Ļ
electrons of the <i>p</i>-benzoquinonemonoimine type, C<sub>6</sub>H<sub>2</sub>(<u>Ā·Ā·Ā·</u>NHR)<sub>2</sub>(<u>Ā·Ā·Ā·</u>O)<sub>2</sub> (R = H (<b>1</b>), <i>n</i>-C<sub>4</sub>H<sub>9</sub> (<b>2</b>), C<sub>3</sub>H<sub>6</sub>āSāCH<sub>3</sub> (<b>3</b>), C<sub>3</sub>H<sub>6</sub>āOāCH<sub>3</sub> (<b>4</b>), CH<sub>2</sub>āC<sub>6</sub>H<sub>5</sub> (<b>5</b>)), adsorbed on Au. These molecules are stable
zwitterions by virtue of the meta positions occupied by the nitrogen
and oxygen substituents on the central ring, respectively. The structures
of <b>2</b>ā<b>4</b> have been determined by single
crystal X-ray diffraction and indicate that in these molecules, two
chemically connected but electronically not conjugated 6Ļ electron
subunits are present, which explains their strong dipolar character.
We systematically observed that homogeneous molecular films with thickness
as small as 1 nm were formed on Au, which fully cover the surface,
even for a variety of R substituents. Preferential adsorption toward
the patterned gold areas on SiO<sub>2</sub> substrates was found with <b>4</b>. Optimum self-assembling of <b>2</b> and <b>5</b> results in ordered close packed films, which exhibit n-type character,
based on the position of the Fermi level close to the conduction band
minimum, suggesting high conductivity properties. This new type of
self-assembled molecular films offers interesting possibilities for
engineering metalāorganic interfaces, of critical importance
for organic electronics
Toward Ferroelectric Control of Monolayer MoS<sub>2</sub>
The
chemical vapor deposition (CVD) of molybdenum disulfide (MoS<sub>2</sub>) single-layer films onto periodically poled lithium niobate is possible
while maintaining the substrate polarization pattern. The MoS<sub>2</sub> growth exhibits a preference for the ferroelectric domains
polarized āupā with respect to the surface so that the
MoS<sub>2</sub> film may be templated by the substrate ferroelectric
polarization pattern without the need for further lithography. MoS<sub>2</sub> monolayers preserve the surface polarization of the āupā
domains, while slightly quenching the surface polarization on the
ādownā domains as revealed by piezoresponse force microscopy.
Electrical transport measurements suggest changes in the dominant
carrier for CVD MoS<sub>2</sub> under application of an external voltage,
depending on the domain orientation of the ferroelectric substrate.
Such sensitivity to ferroelectric substrate polarization opens the
possibility for ferroelectric nonvolatile gating of transition metal
dichalcogenides in scalable devices fabricated free of exfoliation
and transfer
Surface Electronic Structure of Hybrid Organo Lead Bromide Perovskite Single Crystals
The electronic structure and band
dispersion of methylammonium
lead bromide, CH<sub>3</sub>NH<sub>3</sub>PbBr<sub>3</sub>, has been
investigated through a combination of angle-resolved photoemission
spectroscopy (ARPES) and inverse photoemission spectroscopy (IPES),
as well as theoretical modeling based on density functional theory.
The experimental band structures are consistent with the density functional
calculations. The results demonstrate the presence of a dispersive
valence band in MAPbBr<sub>3</sub> that peaks at the MĢ
point
of the surface Brillouin zone. The results also indicate that the
surface termination of the CH<sub>3</sub>NH<sub>3</sub>PbBr<sub>3</sub> is the methylammonium bromide (CH<sub>3</sub>NH<sub>3</sub>Br) layer.
We find our results support models that predict a heavier hole effective
mass in the region of ā0.23 to ā0.26 m<sub>e</sub>,
along the ĪĢ
(surface Brillouin center) to MĢ
point
of the surface Brillouin zone. The surface appears to be n-type as
a result of an excess of lead in the surface region
Gold Dispersion and Activation on the Basal Plane of Single-Layer MoS<sub>2</sub>
Gold
islands are typically associated with high binding affinity
to adsorbates and catalytic activity. Here we present the growth of
dispersed nanoscale gold islands on single layer MoS<sub>2</sub>,
prepared on an inert SiO<sub>2</sub>/Si support by chemical vapor
deposition. This study offers a combination of growth process development,
optical characterization, photoelectron spectroscopy at submicron
spatial resolution, and advanced density functional theory modeling
for detailed insight into the electronic interaction between gold
and single-layer MoS<sub>2</sub>. In particular, we find the gold
density of states in Au/MoS<sub>2</sub>/SiO<sub>2</sub>/Si to be far
less well-defined than Au islands on other 2-dimensional materials
such as graphene, for which we also provide data. We attribute this
effect to the presence of heterogeneous Au adatom/MoS<sub>2</sub>-support
interactions within the nanometer-scale gold cluster. Theory predicts
that CO will exhibit adsorption energies in excess of 1 eV at the
Au cluster edges, where the local density of states is dominated by
Au 5d<sub><i>z</i></sub>2 symmetry