2 research outputs found
Temperature Dependence of the Band Gap of CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> Stabilized with PMMA: A Modulated Surface Photovoltage Study
CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> layers chemically stabilized
with polyÂ(methyl methacrylate) (PMMA), relevant for photovoltaic
applications, have been investigated by modulated surface photovoltage
(SPV) spectroscopy at temperatures (<i>T</i>) between â182
and 60 °C. SPV is sensitive only to the PMMA/CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> interface region where photogeneration and
charge separation take place. The <i>T</i> dependencies
of the Tauc gap (<i>E</i><sub>gâTauc</sub>, equivalent
to absorption measurements) and of the gap determined from the maximum
slope (<i>E</i><sub>gâtp</sub>, almost at increased
absorption) were analyzed on the basis of the in-phase SPV spectra.
At 32 °C, the values of <i>E</i><sub>gâTauc</sub> and <i>E</i><sub>gâtp</sub> were 1.540 and 1.560
eV, respectively. A jump of <i>E</i><sub>gâTauc</sub> and <i>E</i><sub>gâtp</sub> by 10 meV at 40 °C
was interpreted as the transition from the tetragonal to the cubic
phase at <i>T</i> lower than values known from literature. <i>E</i><sub>gâTauc</sub> and <i>E</i><sub>gâtp</sub> of the cubic phase decreased with increasing <i>T</i>.
In contrast, <i>E</i><sub>gâTauc</sub> and <i>E</i><sub>gâtp</sub> of the tetragonal phase decreased
moderately with decreasing <i>T</i> to 1.528 and 1.546 eV
at â182 °C, respectively. No signature has been observed
in <i>E</i><sub>gâTauc</sub> and <i>E</i><sub>gâtp</sub> for the transition from the tetragonal to
the orthorhombic phase. Structural interactions at PMMA/CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> interfaces seem important for phase
transitions in CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> layers
Self-Assembled, Stabilizer-Free ZnS Nanodot Films Using Spray-Based Approaches
A direct
self-assembly of high-quality, uncoated ZnS nanodots on a given substrate
was obtained using two techniques: the sequential and cyclic spray
ion layer gas reaction (spray-ILGAR) as well as the simultaneous and
continuous spray chemical vapor deposition (spray-CVD). The spray-ILGAR
nanodots are homogeneous in size (3â6 nm), regular in shape,
and uniform in composition, while the spray-CVD nanodots are larger
and irregular in shape with inclusions of ZnO. By employing these
two spray-based techniques, the synthesis of nanodots directly assembled
on the substrate surface can be realized in a controlled manner, covering
a certain range of compositions, tunable sizes, and controllable interparticle
distances. <i>In situ</i> mass spectrometry was implemented
in the real-time process in order to achieve better understanding
of the intrinsic chemistry involved. We systematically study the influence
of the process parameters on the formation of the nanodots and compare
the morphology, composition, and property of the obtained nanodots.
Based on these investigations, the underlying mechanism that controls
the special growth of the nanodots in spray-ILGAR and spray-CVD processes
is proposed. It can account for the similarities and differences of
these two kinds of nanodots. A passivation/point contact bilayer,
composed of the spray-based ZnS nanodots covered by a homogeneous
ILGAR In<sub>2</sub>S<sub>3</sub> layer, is used as the buffer in
the chalcopyrite solar cells, resulting in the cell performance improvement
compared to the pure ILGAR In<sub>2</sub>S<sub>3</sub> buffer