17 research outputs found
Stereochemically Active Lone Pairs and Nonlinear Optical Properties of Two-Dimensional Multilayered Tin and Germanium Iodide Perovskites
Two-dimensional (2D) metal halide perovskites are promising
tunable
semiconductors. Previous studies have focused on Pb-based structures,
whereas the multilayered Sn- and Ge-based analogues are largely unexplored,
even though they potentially exhibit more diverse structural chemistry
and properties associated with the more polarizable ns2 lone-pair electrons. Herein, we report the synthesis
and structures of 2D tin iodide perovskites (BA)2(A)Sn2I7, where BA = n-butylammonium
and A = methylammonium, formamidinium, dimethylammonium, guanidinium,
or acetamidinium, and those of 2D germanium iodide perovskites (BA)2(A)Ge2I7, where A = methylammonium or
formamidinium. By comparing these structures along with their Pb counterparts,
we establish correlations between the effect of group IV-cationās
lone-pair stereochemical activity on the perovskite crystal structures
and the resulting semiconducting properties such as bandgaps and carrierāphonon
interactions and nonlinear optical properties. We find that the strength
of carrierāphonon interaction increases with increasing lone-pair
activity, leading to a more prominent photoluminescence tail on the
low-energy side. Moreover, (BA)2(A)Ge2I7 exhibit strong second harmonic generation with second-order
nonlinear coefficients of ā¼10 pm Vā1 that
are at least 10 times those of Sn counterparts and 100 times those
of Pb counterparts. We also report the third-order two-photon absorption
coefficients of (BA)2(A)Sn2I7 to
be ā¼10 cm MWā1, which are one order of magnitude
larger than those of the Pb counterparts and traditional inorganic
semiconductors. These results not only highlight the role of lone-pair
activity in linking the compositions and physical properties of 2D
halide perovskites but also demonstrate 2D tin and germanium iodide
perovskites as promising lead-free alternatives for nonlinear optoelectronic
devices
Visualization and Studies of Ion-Diffusion Kinetics in Cesium Lead Bromide Perovskite Nanowires
The facile chemical
transformation of metal halide perovskites
via ion exchange has been attributed to their āsoftā
crystal lattices that enable fast ion migration. Kinetic studies of
such processes could provide mechanistic insights on the ion migration
dynamics. Herein, by using aligned single-crystal nanowires of cesium
lead bromide (CsPbBr<sub>3</sub>) perovskite on epitaxial substrates
as platforms, we visualize and investigate the cation or anion interdiffusion
kinetics via spatially resolved photoluminescence measurement on heterostructures
fabricated by stacking CsPbCl<sub>3</sub>, MAPbI<sub>3</sub>, or MAPbBr<sub>3</sub> microplates on top of CsPbBr<sub>3</sub> nanowires. Time-dependent
confocal photoluminescence microscopy and energy-dispersive X-ray
spectroscopy showed the solid-state anion interdiffusion readily occurs
to result in halide concentration gradients along CsPbBr<sub>3ā3<i>x</i></sub>Cl<sub>3<i>x</i></sub> (<i>x</i> = 0ā1) nanowires. Quantitative analysis of such composition
profiles using Fickās law allowed us, for the first time, to
extract interdiffusion coefficients of the chloride-bromide couple
and an activation energy of 0.44 ± 0.02 eV for ion diffusion
from temperature-dependent studies. In contrast, iodide-bromide interdiffusion
is limited, likely due to the complex phase behaviors of mixed alloys
of CsPbĀ(Br,I)<sub>3</sub>. In contrast to the relatively mobile anions,
A-site cation interdiffusion across the MAPbBr<sub>3</sub>/CsPbBr<sub>3</sub> junctions was barely observed at room temperature. Our results
present a general method to investigate the kinetics of the solid-state
ion migration, and the gained insights on ion diffusion can provide
guidelines for rationally designing perovskite heterostructures that
could lead to new properties for fundamental studies and technological
applications
Visualization and Studies of Ion-Diffusion Kinetics in Cesium Lead Bromide Perovskite Nanowires
The facile chemical
transformation of metal halide perovskites
via ion exchange has been attributed to their āsoftā
crystal lattices that enable fast ion migration. Kinetic studies of
such processes could provide mechanistic insights on the ion migration
dynamics. Herein, by using aligned single-crystal nanowires of cesium
lead bromide (CsPbBr<sub>3</sub>) perovskite on epitaxial substrates
as platforms, we visualize and investigate the cation or anion interdiffusion
kinetics via spatially resolved photoluminescence measurement on heterostructures
fabricated by stacking CsPbCl<sub>3</sub>, MAPbI<sub>3</sub>, or MAPbBr<sub>3</sub> microplates on top of CsPbBr<sub>3</sub> nanowires. Time-dependent
confocal photoluminescence microscopy and energy-dispersive X-ray
spectroscopy showed the solid-state anion interdiffusion readily occurs
to result in halide concentration gradients along CsPbBr<sub>3ā3<i>x</i></sub>Cl<sub>3<i>x</i></sub> (<i>x</i> = 0ā1) nanowires. Quantitative analysis of such composition
profiles using Fickās law allowed us, for the first time, to
extract interdiffusion coefficients of the chloride-bromide couple
and an activation energy of 0.44 ± 0.02 eV for ion diffusion
from temperature-dependent studies. In contrast, iodide-bromide interdiffusion
is limited, likely due to the complex phase behaviors of mixed alloys
of CsPbĀ(Br,I)<sub>3</sub>. In contrast to the relatively mobile anions,
A-site cation interdiffusion across the MAPbBr<sub>3</sub>/CsPbBr<sub>3</sub> junctions was barely observed at room temperature. Our results
present a general method to investigate the kinetics of the solid-state
ion migration, and the gained insights on ion diffusion can provide
guidelines for rationally designing perovskite heterostructures that
could lead to new properties for fundamental studies and technological
applications
Carrier Decay Properties of Mixed Cation FormamidiniumāMethylammonium Lead Iodide Perovskite [HC(NH<sub>2</sub>)<sub>2</sub>]<sub>1ā<i>x</i></sub>[CH<sub>3</sub>NH<sub>3</sub>]<sub><i>x</i></sub>PbI<sub>3</sub> Nanorods
Organicāinorganic
lead iodide perovskites are efficient
materials for photovoltaics and light-emitting diodes. We report carrier
decay dynamics of nanorods of mixed cation formamidinium and methylammonium
lead iodide perovskites [HCĀ(NH<sub>2</sub>)<sub>2</sub>]<sub>1ā<i>x</i></sub>[CH<sub>3</sub>NH<sub>3</sub>]<sub><i>x</i></sub>PbI<sub>3</sub> (FA<sub>1ā<i>x</i></sub>MA<sub><i>x</i></sub>PbI<sub>3</sub>) synthesized through a simple
solution method. The structure and FA/MA composition ratio of the
single-crystal FA<sub>1ā<i>x</i></sub>MA<sub><i>x</i></sub>PbI<sub>3</sub> nanorods are fully characterized,
which shows that the mixed cation FA<sub>1ā<i>x</i></sub>MA<sub><i>x</i></sub>PbI<sub>3</sub> nanorods are
stabilized in the perovskite structure. The photoluminescence (PL)
emission from FA<sub>1ā<i>x</i></sub>MA<sub><i>x</i></sub>PbI<sub>3</sub> nanorods continuously shifts from
821 to 782 nm as the MA ratio (<i>x</i>) increases from
0 to 1 and is shown to be inhomogeneously broadened. Time-resolved
PL from individual FA<sub>1ā<i>x</i></sub>MA<sub><i>x</i></sub>PbI<sub>3</sub> nanorods demonstrates that
lifetimes of mixed cation FA<sub>1ā<i>x</i></sub>MA<sub><i>x</i></sub>PbI<sub>3</sub> nanorods are longer
than those of the pure FAPbI<sub>3</sub> or MAPbI<sub>3</sub> nanorods,
and the FA<sub>0.4</sub>MA<sub>0.6</sub>PbI<sub>3</sub> displays the
longest average PL lifetime of about 2 μs. These results suggest
that mixed cation FA<sub>1ā<i>x</i></sub>MA<sub><i>x</i></sub>PbI<sub>3</sub> perovskites are promising for high-efficiency
photovoltaics and other optoelectronic applications
Photocurrent Mapping in Single-Crystal Methylammonium Lead Iodide Perovskite Nanostructures
We
investigate solution-grown single-crystal methylammonium lead iodide
(MAPbI<sub>3</sub>) nanowires and nanoplates with spatially resolved
photocurrent mapping. Sensitive perovskite photodetectors with Schottky
contacts are fabricated by directly transferring the nanostructures
on top of prepatterned gold electrodes. Scanning photocurrent microscopy
(SPCM) measurements on these single-crystal nanostructures reveal
a minority charge carrier diffusion length up to 21 μm, which
is significantly longer than the values observed in polycrystalline
MAPbI<sub>3</sub> thin films. When the excitation energy is close
to the bandgap, the photocurrent becomes substantially stronger at
the edges of nanostructures, which can be understood by the enhancement
of light coupling to the nanostructures. These perovskite nanostructures
with long carrier diffusion lengths and strong photonic enhancement
not only provide an excellent platform for studying their intrinsic
properties but may also boost the performance of perovskite-based
optoelectronic devices
High-Performance Electrocatalysis for Hydrogen Evolution Reaction Using Se-Doped Pyrite-Phase Nickel Diphosphide Nanostructures
The study of efficient, robust, and
earth-abundant electrocatalysts
for the hydrogen evolution reaction (HER) is essential for hydrogen-based
energy technologies. Previous works have demonstrated that pyrite-structure
materials (e.g., CoS<sub>2</sub>, NiSe<sub>2</sub>) are efficient
HER catalysts. Here, we first systematically investigate the nanostructure
synthesis of a series of pyrite-phase nickel phosphoselenide materialsīøNiP<sub>2</sub>, Se-doped NiP<sub>2</sub> (NiP<sub>1.93</sub>Se<sub>0.07</sub>), P-doped NiSe<sub>2</sub> (NiP<sub>0.09</sub>Se<sub>1.91</sub>),
and NiSe<sub>2</sub>īøthrough a facile thermal conversion of
NiĀ(OH)<sub>2</sub> nanoflakes. The similar nanostructures enable a
systematic and fair comparison of their structural properties and
catalytic activities for HER. We found that NiP<sub>1.93</sub>Se<sub>0.07</sub> shows the best HER performance, followed by NiP<sub>2</sub>, NiP<sub>0.09</sub>Se<sub>1.91</sub>, and NiSe<sub>2</sub>. Se-doped
NiP<sub>2</sub> grown on carbon fiber paper can achieve an electrocatalytic
current density of 10 mA cm<sup>ā2</sup> at an overpotential
as low as 84 mV and a small Tafel slope of 41 mV decade<sup>ā1</sup>. This study not only estabilishes Se-doped NiP<sub>2</sub> as a
competitive HER catalyst, but also demonstrates that doping or alloying
of developed catalysts (especially doping with anions from another
group; e.g., selenium to phosphorus) can improve the HER catalytic
activity, which provides a general strategy to improve catalytic efficiencies
of existing electrocatalysts for HER
Broad Wavelength Tunable Robust Lasing from Single-Crystal Nanowires of Cesium Lead Halide Perovskites (CsPbX<sub>3</sub>, X = Cl, Br, I)
Lead halide perovskite
nanowires (NWs) are emerging as a class
of inexpensive semiconductors with broad bandgap tunability for optoelectronics,
such as tunable NW lasers. Despite exciting progress, the current
organicāinorganic hybrid perovskite NW lasers suffer from limited
tunable wavelength range and poor material stability. Herein, we report
facile solution growth of single-crystal NWs of inorganic perovskite
CsPbX<sub>3</sub> (X = Br, Cl) and their alloys [CsPbĀ(Br,Cl)<sub>3</sub>] and a low-temperature vapor-phase halide exchange method to convert
CsPbBr<sub>3</sub> NWs into perovskite phase CsPbĀ(Br,I)<sub>3</sub> alloys and metastable CsPbI<sub>3</sub> with well-preserved perovskite
crystal lattice and NW morphology. These single crystalline NWs with
smooth end facets and subwavelength dimensions are ideal FabryāPerot
cavities for NW lasers. Optically pumped tunable lasing across the
entire visible spectrum (420ā710 nm) is demonstrated at room
temperature from these NWs with low lasing thresholds and high-quality
factors. Such highly efficient lasing similar to what can be achieved
with organicāinorganic hybrid perovskites indicates that organic
cation is not essential for light emission application from these
lead halide perovskite materials. Furthermore, the CsPbBr<sub>3</sub> NW lasers show stable lasing emission with no measurable degradation
after at least 8 h or 7.2 Ć 10<sup>9</sup> laser shots under
continuous illumination, which are substantially more robust than
their organicāinorganic counterparts. The Cs-based perovskites
offer a stable material platform for tunable NW lasers and other nanoscale
optoelectronic devices
Additional file 1 of Multi-faceted analysis reveals the characteristics of silk fabrics on a Liao Dynasty DieXie belt
Additional file 1. Supplementary material
Two-Dimensional Lead Halide Perovskites Templated by a Conjugated Asymmetric Diammonium
We
report novel two-dimensional lead halide perovskite structures templated
by a unique conjugated aromatic dication, <i>N</i>,<i>N</i>-dimethylphenylene-<i>p</i>-diammonium (DPDA).
The asymmetrically substituted primary and tertiary ammoniums in DPDA
facilitate the formation of two-dimensional network (2DN) perovskite
structures incorporating a conjugated dication between the PbX<sub>4</sub><sup>2ā</sup> (X = Br, I) layers. These 2DN structures
of (DPDA)ĀPbI<sub>4</sub> and (DPDA)ĀPbBr<sub>4</sub> were characterized
by single-crystal X-ray diffraction, showing uniquely low distortions
in the PbāXāPb bond angle for 2D perovskites. The PbāIāPb
bond angle is very close to ideal (180°) for a 2DN lead iodide
perovskite, which can be attributed to the ability of the rigid diammonium
DPDA to insert into the PbX<sub>6</sub><sup>2ā</sup> octahedral
pockets. Optical characterization of (DPDA)ĀPbI<sub>4</sub> shows an
excitonic absorption peak at 2.29 eV (541 nm), which is red-shifted
in comparison to similar 2DN lead iodide structures. Temperature-dependent
photoluminescence of both compounds reveals both a self-trapped exciton
and free exciton emission feature. The reduced exciton absorption
energy and emission properties are attributed to the dication-induced
structural order of the inorganic PbX<sub>4</sub><sup>2ā</sup> layers. DFT calculation results suggest mixing of the conjugated
organic orbital component in the valence band of these 2DN perovskites.
These results demonstrate a rational new strategy to incorporate conjugated
organic dications into hybrid perovskites and will spur spectroscopic
investigations of these compounds as well as optoelectronic applications