8 research outputs found
Charge Transfer at the PTCDA/Black Phosphorus Interface
The
interfacial electronic structure at the organic–inorganic
semiconductor interface plays an important role in determining the
electrical and optical performance of organic-based devices. Here,
we studied the molecular alignment and electronic structure of thermally
deposited 3,4,9,10-perylene-tetracarboxylic-dianhydride (PTCDA) molecules
on cleaved black phosphorus using photoelectron spectroscopy. The
work function of black phosphorus is substantially upped with an organic
thin film, originating from the charge transfer from black phosphorus
to PTCDA. According to our photoemission spectrum and theoretical
simulation, we also define the interaction between PTCDA and black
phosphorus as weak van de Waals physisorption, rather than bonding
chemisorption. Furthermore, we show that PTCDA thin film can effectively
isolate reactive oxygen species, thereby protecting BP surface oxidation
and deterioration under ambient conditions. Our results suggest the
possibility of manipulating interfacial electronic structures of black
phosphorus interface by noncovalent with organic semiconductor, in
particular for applications in high-performance organic–inorganic
hybrid photovoltaic
Effects of Precursor Ratios and Annealing on Electronic Structure and Surface Composition of CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> Perovskite Films
The electronic structure and surface
composition of CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> (MAPbI<sub>3</sub>) films fabricated
by one-step method with different precursor ratios of PbI<sub>2</sub> to CH<sub>3</sub>NH<sub>3</sub>I (PbI<sub>2</sub>/MAI) have been
investigated with ultraviolet photoelectron spectroscopy (UPS) and
X-ray photoelectron spectroscopy (XPS). It is found that the core
levels of all components in the MAPbI<sub>3</sub> film shift toward
lower binding energy with decreasing the precursor ratio of PbI<sub>2</sub>/MAI, indicating that the electronic structures of the MAPbI<sub>3</sub> film can be adjusted by the precursor ratio of PbI<sub>2</sub>/MAI. The elemental compositions of the MAPbI<sub>3</sub> film also
depend on the precursor ratio and annealing process, and the compositions
are strongly correlated to the electronic properties of the films.
The electronic properties remain unchanged with an annealing at 110
°C. However, a core level shift of 0.5 eV toward higher binding
energy is observed with an annealing at 150 °C, together with
noticeable composition change from the XPS core level analysis. The
distribution of all chemical components in the MAPbI<sub>3</sub> film
is further investigated with angle-resolved XPS (AR-XPS). It is observed
that annealing at 150 °C leads to relatively shallow distribution
variations of I and Pb in the MAPbI<sub>3</sub> film, accompanied
by infiltration of metallic Pb into the bulk
Interface Electronic Structure between Au and Black Phosphorus
The
interface electronic structure between Au and black phosphorus
has been investigated with ultraviolet and X-ray photoemission spectroscopy.
We observed that Au clusters form at the initial Au deposition, and
an interface dipole is observed at the interface between Au and BP.
The outermost BP lattice is destroyed and unbonded P appears, which
is due to the formation of metallic Au by the deposition of more than
8 Å Au. The unbonded P is surface segregated at 8–15 Å,
and it is covered with further increasing of the Au thickness. These
observations reveal the processes in the Au/BP interface and provide
possible directions to fabricate high performance Au/BP-based device
From Water Oxidation to Reduction: Transformation from Ni<sub><i>x</i></sub>Co<sub>3–<i>x</i></sub>O<sub>4</sub> Nanowires to NiCo/NiCoO<sub><i>x</i></sub> Heterostructures
A homologous
Ni–Co based nanowire catalyst pair, composed of Ni<sub><i>x</i></sub>Co<sub>3–<i>x</i></sub>O<sub>4</sub> nanowires and NiCo/NiCoO<sub><i>x</i></sub> nanohybrid,
is developed for efficient overall water splitting. Ni<sub><i>x</i></sub>Co<sub>3–<i>x</i></sub>O<sub>4</sub> nanowires are found as a highly active oxygen evolution reaction
(OER) catalyst, and they are converted into a highly active hydrogen
evolution reaction (HER) catalyst through hydrogenation treatment
as NiCo/NiCoO<sub><i>x</i></sub> heteronanostructures. An
OER current density of 10 mA cm<sup>–2</sup> is obtained with
the Ni<sub><i>x</i></sub>Co<sub>3–<i>x</i></sub>O<sub>4</sub> nanowires under an overpotential of 337 mV in
1.0 M KOH, and an HER current density of 10 mA cm<sup>–2</sup> is obtained with the NiCo/NiCoO<sub><i>x</i></sub> heteronanostructures
at an overpotential of 155 mV. When integrated in an electrolyzer,
these catalysts demonstrate a stable performance in water splitting
CuSbS<sub>2</sub> as a Promising Earth-Abundant Photovoltaic Absorber Material: A Combined Theoretical and Experimental Study
Recently,
CuSbS<sub>2</sub> has been proposed as an alternative
earth-abundant absorber material for thin film solar cells. However,
no systematic study on the chemical, optical, and electrical properties
of CuSbS<sub>2</sub> has been reported. Using density functional theory
(DFT) calculations, we showed that CuSbS<sub>2</sub> has superior
defect physics with extremely low concentration of recombination-center
defects within the forbidden gap, espeically under the S rich condition.
It has intrinsically p-type conductivity, which is determined by the
dominant Cu vacancy (<i>V</i><sub>Cu</sub>) defects with
the a shallow ionization level and the lowest formation energy. Using
a hydrazine based solution process, phase-pure, highly crystalline
CuSbS<sub>2</sub> film with large grain size was successfully obtained.
Optical absorption investigation revealed that our CuSbS<sub>2</sub> has a direct band gap of 1.4 eV. Ultraviolet photoelectron spectroscopy
(UPS) study showed that the conduction band and valence band are located
at 3.85 eV and −5.25 eV relative to the vacuum level, respectively.
As the calculations predicted, a p-type conductivity is observed in
the Hall effect measurements with a hole concentration of ∼10<sup>18</sup> cm<sup>–3</sup> and hole mobility of 49 cm<sup>2</sup>/(V s). Finally, we have built a prototype FTO/CuSbS<sub>2</sub>/CdS/ZnO/ZnO:Al/Au
solar cell and achieved 0.50% solar conversion efficiency. Our theoretical
and experimental investigation confirmed that CuSbS<sub>2</sub> is
indeed a very promising absorber material for solar cell application
Modification of Ultrathin NPB Interlayer on the Electronic Structures of the CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub>/NPB/MoO<sub>3</sub> Interface
Modification
of the ultrathin <i>N</i>,<i>N</i>′-DiÂ(1-naphthyl)-<i>N</i>,<i>N</i>′-diphenyl-(1,1′-biphenyl)-4,4′-diamine
(NPB) insertion layer on the electronic structures of the CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> (MAPbI<sub>3</sub>)/MoO<sub>3</sub> interfaces is investigated using ultraviolet photoelectron spectroscopy
(UPS) and X-ray photoelectron spectroscopy (XPS). It is found that
when an ultrathin NPB insertion layer of 16 Ã… is inserted between
MAPbI<sub>3</sub> and MoO<sub>3</sub>, the chemical reaction between
the latter two can be effectively suppressed, and a favorable energy-level
alignment is achieved. The valence band maximum (VBM) or highest occupied
molecular orbital (HOMO) at the MAPbI<sub>3</sub>/NPB/MoO<sub>3</sub> interface facilitates the hole transportation from the MAPbI<sub>3</sub> layer through the NPB layer toward the NPB/MoO<sub>3</sub> interface. As a result, the holes can be efficiently extracted to
the hole collection electrode due to the small energy offset between
the conduction band minimum (CBM) of MoO<sub>3</sub> and the HOMO
of NPB. Therefore, the modification by the ultrathin NPB interlayer
on the electronic structures of the MAPbI<sub>3</sub>/MoO<sub>3</sub> interface can greatly improve the hole extraction and thus enhance
the power efficiency of the corresponding solar cells
Thermal Evaporation and Characterization of Sb<sub>2</sub>Se<sub>3</sub> Thin Film for Substrate Sb<sub>2</sub>Se<sub>3</sub>/CdS Solar Cells
Sb<sub>2</sub>Se<sub>3</sub> is a promising absorber material for
photovoltaic cells because of its optimum band gap, strong optical
absorption, simple phase and composition, and earth-abundant and nontoxic
constituents. However, this material is rarely explored for photovoltaic
application. Here we report Sb<sub>2</sub>Se<sub>3</sub> solar cells
fabricated from thermal evaporation. The rationale to choose thermal
evaporation for Sb<sub>2</sub>Se<sub>3</sub> film deposition was first
discussed, followed by detailed characterization of Sb<sub>2</sub>Se<sub>3</sub> film deposited onto FTO with different substrate temperatures.
We then studied the optical absorption, photosensitivity, and band
position of Sb<sub>2</sub>Se<sub>3</sub> film, and finally a prototype
photovoltaic device FTO/Sb<sub>2</sub>Se<sub>3</sub>/CdS/ZnO/ZnO:Al/Au
was constructed, achieving an encouraging 2.1% solar conversion efficiency
Interfacial Electronic Structures of Photodetectors Based on C8BTBT/Perovskite
Comprehensive
measurements of ultraviolet photoemission spectroscopy, X-ray photoemission
spectroscopy, X-ray diffraction, and atomic force microscopy are adopted
to investigate the corelevance of energy level alignment, molecular
orientation, and film growth of Au/C8BTBT/perovskite interfaces. A
small energy offset of valence band maximum of 0.06 eV between perovskite
and C8BTBT makes hole transportation feasible. About 0.65 eV upward
shift of energy levels is observed with the deposition of the Au film
on C8BTBT, which enhances hole transportation to the Au electrode.
The observations from the interface analysis are supported by a prototype
photodetector of Au (80 nm)/C8BTBT (20 nm)/perovskite (100 nm) that
exhibits excellent performances whose responsivity can reach up to
2.65 A W<sup>–1</sup>, 4 times higher than the best CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> photodetectors