3 research outputs found
Pressure-Induced Phase Transition of Hydrogen Storage Material Hydrazine Bisborane: Evolution of Dihydrogen Bonds
We report the high-pressure behavior
of dihydrogen-bonded hydrogen
storage material hydrazine bisborane (BH<sub>3</sub>N<sub>2</sub>H<sub>4</sub>BH<sub>3</sub>, HBB) via in situ angle-dispersive X-ray diffraction
(ADXRD) and Raman spectroscopy in a diamond anvil cell up to 2.0 GPa.
A reversible phase transition at 0.4 GPa was confirmed by ADXRD experiments.
The Rietveld refinement showed the high-pressure phase was consistent
with the crystal structure of α′-phase (low-temperature
phase). Through the analysis of structure changes, Raman spectroscopy,
and the Hirshfeld surface, we studied the evolution of dihydrogen
bonds under high pressure and attributed the pressure-induced phase
transition to the distortion and rotation of the NH<sub>2</sub>–NH<sub>2</sub> group. This work will further the understanding of the characteristics
of dihydrogen bonds and provide some contribution to future hydrogen
storage applications of HBB
Pressure-Tailored Band Gap Engineering and Structure Evolution of Cubic Cesium Lead Iodide Perovskite Nanocrystals
Metal
halide perovskites (MHPs) have attracted increasing research
attention given the ease of solution processability with excellent
optical absorption and emission qualities. However, effective strategies
for engineering the band gap of MHPs to satisfy the requirements of
practical applications are difficult to develop. Cubic cesium lead
iodide (α-CsPbI<sub>3</sub>), a typical MHP with an ideal band
gap of 1.73 eV, is an intriguing optoelectric material owing to the
approaching Shockley–Queisser limit. Here, we carried out a
combination of in situ photoluminescence, absorption, and angle-dispersive
synchrotron X-ray diffraction spectra to investigate the pressure-induced
optical and structural changes of α-CsPbI<sub>3</sub> nanocrystals
(NCs). The α-CsPbI<sub>3</sub> NCs underwent a phase transition
from cubic (α) to orthorhombic phase and subsequent amorphization
upon further compression. The structural changes with octahedron distortion
to accommodate the Jahn–Teller effect were strongly responsible
for the optical variation with the increase of pressure. First-principles
calculations reveal that the band-gap engineering is governed by orbital
interactions within the inorganic Pb–I frame through the structural
modification. Our high-pressure studies not only established structure–property
relationships at the atomic scale of α-CsPbI<sub>3</sub> NCs,
but also provided significant clues in optimizing photovoltaic performance,
thus facilitating the design of novel MHPs with increased stimulus-resistant
capability
Pressure Effects on Structure and Optical Properties in Cesium Lead Bromide Perovskite Nanocrystals
Metal
halide perovskites (MHPs) are gaining increasing interest
because of their extraordinary performance in optoelectronic devices
and solar cells. However, developing an effective strategy for achieving
the band-gap engineering of MHPs that will satisfy the practical applications
remains a great challenge. In this study, high pressure is introduced
to tailor the optical and structural properties of MHP-based cesium
lead bromide nanocrystals (CsPbBr<sub>3</sub> NCs), which exhibit
excellent thermodynamic stability. Both the pressure-dependent steady-state
photoluminescence and absorption spectra experience a stark discontinuity
at ∼1.2 GPa, where an isostructural phase transformation regarding
the <i>Pbnm</i> space group occurs. The physical origin
points to the repulsive force impact due to the overlap between the
valence electron charge clouds of neighboring layers. Simultaneous
band-gap narrowing and carrier-lifetime prolongation of CsPbBr<sub>3</sub> trihalide perovskite NCs were also achieved as expected,
which facilitates the broader solar spectrum absorption for photovoltaic
applications. Note that the values of the phase change interval and
band-gap red-shift of CsPbBr<sub>3</sub> nanowires are between those
for CsPbBr<sub>3</sub> nanocubes and the corresponding bulk counterparts,
which results from the unique geometrical morphology effect. First-principles
calculations unravel that the band-gap engineering is governed by
orbital interactions within the inorganic Pb–Br frame through
structural modification. Changes of band structures are attributed
to the synergistic effect of pressure-induced modulations of the Br–Pb
bond length and Pb–Br–Pb bond angle for the PbBr<sub>6</sub> octahedral framework. Furthermore, the significant distortion
of the lead–bromide octahedron to accommodate the Jahn–Teller
effect at much higher pressure would eventually lead to a direct to
indirect band-gap electronic transition. This study enables high pressure
as a robust tool to control the structure and band gap of CsPbBr<sub>3</sub> NCs, thus providing insight into the microscopic physiochemical
mechanism of these compressed MHP nanosystems